From 6279fa19ac6e2a4087df2e6fe985430ecc2c2d5d Mon Sep 17 00:00:00 2001 From: kinitrupti Date: Fri, 12 May 2017 18:53:46 +0530 Subject: Removed duplicates --- .../Chapter1.ipynb | 311 --------------- .../Chapter10.ipynb | 434 --------------------- .../Chapter10_1.ipynb | 434 --------------------- .../Chapter10_2.ipynb | 434 --------------------- .../Chapter11.ipynb | 114 ------ .../Chapter11_1.ipynb | 114 ------ .../Chapter11_2.ipynb | 114 ------ .../Chapter12.ipynb | 285 -------------- .../Chapter12_1.ipynb | 285 -------------- .../Chapter12_2.ipynb | 285 -------------- .../Chapter13.ipynb | 250 ------------ .../Chapter13_1.ipynb | 250 ------------ .../Chapter13_2.ipynb | 250 ------------ .../Chapter14.ipynb | 107 ----- .../Chapter14_1.ipynb | 107 ----- .../Chapter14_2.ipynb | 107 ----- .../Chapter15.ipynb | 203 ---------- .../Chapter15_1.ipynb | 203 ---------- .../Chapter15_2.ipynb | 203 ---------- .../Chapter16.ipynb | 114 ------ .../Chapter16_1.ipynb | 114 ------ 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backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter9_2.ipynb (limited to 'backup/Modern_Physics_By_G.Aruldas_version_backup') diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter1.ipynb deleted file mode 100755 index 483d55f3..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter1.ipynb +++ /dev/null @@ -1,311 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:467ef5c6562d2c93b60e422b9b9a8c5a34323da84f6c33e87f513c3c578db36d" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "1: The special theory of relativity" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.2, Page number 10" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=1; #assume\n", - "udash=0.9*c; #speed of 2nd rocket\n", - "v=0.6*c; #speed of 1st rocket\n", - "\n", - "#Calculation\n", - "u1=(udash+v)/(1+(udash*v/(c**2))); #speed of 2nd rocket in same direction\n", - "u2=(-udash+v)/(1-(udash*v/(c**2))); #speed of 2nd rocket in opposite direction\n", - "\n", - "#Result\n", - "print \"speed of 2nd rocket in same direction is\",round(u1,3),\"*c\"\n", - "print \"speed of 2nd rocket in opposite direction is\",round(u2,3),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of 2nd rocket in same direction is 0.974 *c\n", - "speed of 2nd rocket in opposite direction is -0.652 *c\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.3, Page number 12" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "#given L0-L/L0=0.01.so L=0.99*L0\n", - "LbyL0=0.99;\n", - "c=1; #assume\n", - "\n", - "#Calculation\n", - "v2=(c**2)*(1-(LbyL0)**2);\n", - "v=math.sqrt(v2); #speed\n", - "\n", - "#Result\n", - "print \"speed is\",round(v,3),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed is 0.141 *c\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.4, Page number 12" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "delta_tow=2.6*10**-8; #mean lifetime at rest(s)\n", - "d=20; #distance(m)\n", - "c=3*10**8; #speed of light(m/s)\n", - "\n", - "#Calculation\n", - "#delta_t=d/v\n", - "v2=(c**2)/(1+(delta_tow*c/d)**2);\n", - "v=math.sqrt(v2); #speed of unstable particle(m/s)\n", - "\n", - "#Result\n", - "print \"speed of unstable particle is\",round(v/10**8,1),\"*10**8 m/s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of unstable particle is 2.8 *10**8 m/s\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.5, Page number 13" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "delta_t=5*10**-6; #mean lifetime(s)\n", - "c=1; #assume\n", - "v=0.9*c; #speed of beam\n", - "\n", - "#Calculation\n", - "delta_tow=delta_t*math.sqrt(1-(v/c)**2); #proper lifetime of particles(s)\n", - "\n", - "#Result\n", - "print \"proper lifetime of particles is\",round(delta_tow*10**6,2),\"*10**-6 s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "proper lifetime of particles is 2.18 *10**-6 s\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.6, Page number 15" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=1; #assume\n", - "m0bym=100/120; #ratio of masses\n", - "\n", - "#Calculation\n", - "v=c*math.sqrt(1-(m0bym**2)); #speed of body\n", - "\n", - "#Result\n", - "print \"speed of body is\",round(v,3),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of body is 0.553 *c\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.7, Page number 17" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=3*10**8; #speed of light(m/s)\n", - "deltaE=4*10**26; #energy of sun(J/s)\n", - "\n", - "#Calculation\n", - "deltam=deltaE/c**2; #change in mass(kg)\n", - "\n", - "#Result\n", - "print \"change in mass is\",round(deltam/10**9,2),\"*10**9 kg\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "change in mass is 4.44 *10**9 kg\n" - ] - } - ], - "prompt_number": 13 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.8, Page number 17" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=1; #assume\n", - "T=10; #kinetic energy(MeV)\n", - "m0c2=0.512; #rest energy of electron(MeV)\n", - "\n", - "#Calculation\n", - "E=T+m0c2; #total energy(MeV)\n", - "p=math.sqrt((E**2)-(m0c2**2))/c; #momentum of electron(MeV/c)\n", - "v=c*math.sqrt(1-(m0c2/E)**2); #velocity of electron(c)\n", - "\n", - "#Result\n", - "print \"momentum of electron is\",round(p,1),\"MeV/c\"\n", - "print \"velocity of electron is\",round(v,4),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "momentum of electron is 10.5 MeV/c\n", - "velocity of electron is 0.9988 *c\n" - ] - } - ], - "prompt_number": 16 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter10.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter10.ipynb deleted file mode 100755 index d4104917..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter10.ipynb +++ /dev/null @@ -1,434 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:de4c224e2d9bad9e810e24de23e4ee016e17fa0ec4d45805b35802744f1cd3b7" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "10: Crystal structure and bonding" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.5, Page number 213" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h1=1;\n", - "k1=0;\n", - "l1=0; #for (100) plane\n", - "h2=1;\n", - "k2=1;\n", - "l2=1; #for (111) plane\n", - "a=1; #assume\n", - "\n", - "#Calculation\n", - "d100=a/math.sqrt(h1**2+k1**2+l1**2); #spacing between (100) plane\n", - "d111=a/math.sqrt(h2**2+k2**2+l2**2); #spacing between (111) plane\n", - "\n", - "#Result\n", - "print \"spacing between (100) plane is\",d100,\"a\"\n", - "print \"spacing between (111) plane is\",round(d111,3),\"a\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "spacing between (100) plane is 1.0 a\n", - "spacing between (111) plane is 0.577 a\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.6, Page number 213" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "r=0.152; #atomic radius(nm)\n", - "h1=2;\n", - "k1=3;\n", - "l1=1; #for plane (231)\n", - "h2=1;\n", - "k2=1;\n", - "l2=0; #for plane (110)\n", - "\n", - "#Calculation\n", - "a=4*r/math.sqrt(2);\n", - "d231=a/math.sqrt(h1**2+k1**2+l1**2); #spacing between (231) plane(nm) \n", - "d110=a/math.sqrt(h2**2+k2**2+l2**2); #spacing between (110) plane(nm)\n", - "\n", - "#Result\n", - "print \"spacing between (231) plane is\",round(d231,4),\"nm\"\n", - "print \"spacing between (110) plane is\",d110,\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "spacing between (231) plane is 0.1149 nm\n", - "spacing between (110) plane is 0.304 nm\n" - ] - } - ], - "prompt_number": 4 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.7, Page number 213" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=1;\n", - "k=0;\n", - "l=2; #for plane (102)\n", - "a=0.424; #edge(nm)\n", - "\n", - "#Calculation\n", - "d102=a/math.sqrt(h**2+k**2+l**2); #interplanar spacing(nm)\n", - "\n", - "#Result\n", - "print \"interplanar spacing is\",round(d102,4),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "interplanar spacing is 0.1896 nm\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.8, Page number 214" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=3.2*10**-10; #edge(m)\n", - "rho=11.36*10**3; #density(kg/m**3)\n", - "N=6.023*10**26; #avagadro number(per k mol)\n", - "M=207.2; #atomic weight\n", - "\n", - "#Calculation\n", - "n=a**3*rho*N/M; #number of atoms per unit cell\n", - "\n", - "#Result\n", - "print \"number of atoms per unit cell is\",int(n)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number of atoms per unit cell is 1\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.9, Page number 220" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "d=2.51*10**-10; #spacing between planes(m)\n", - "theta=9; #glancing angle(degrees)\n", - "\n", - "#Calculation\n", - "theta=theta*math.pi/180; #glancing angle(radian)\n", - "lamda=2*d*math.sin(theta); #wavelength(m)\n", - "a=lamda/2.51;\n", - "theta2=math.asin(a); #glancing angle for 2nd order diffraction(radian)\n", - "theta2=2*theta*180/math.pi; #glancing angle for 2nd order diffraction(degrees)\n", - "\n", - "#Result\n", - "print \"wavelength of X ray is\",round(lamda*10**10,4),\"angstrom\"\n", - "print \"glancing angle for 2nd order diffraction is\",theta2,\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of X ray is 0.7853 angstrom\n", - "glancing angle for 2nd order diffraction is 18.0 degrees\n" - ] - } - ], - "prompt_number": 28 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.10, Page number 220" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=5*10**-10; #lattice parameter(m)\n", - "n=1;\n", - "lamda=1.4*10**-10; #wavelength(m)\n", - "h=1;\n", - "k=1;\n", - "l=1; #for plane (111)\n", - "\n", - "#Calculation\n", - "d111=a/math.sqrt(h**2+k**2+l**2);\n", - "b=n*lamda/(2*d111);\n", - "theta111=math.asin(b); #incident angle(radian)\n", - "theta111=theta111*180/math.pi; #incident angle(degrees)\n", - "\n", - "#Result\n", - "print \"incident angle is\",int(theta111),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "incident angle is 14 degrees\n" - ] - } - ], - "prompt_number": 30 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.11, Page number 221" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "H=6.626*10**-34; #planck's constant(Js)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "V=120; #potential(V)\n", - "theta=22; #angle(degrees)\n", - "theta=theta*math.pi/180; #angle(radian)\n", - "h=1;\n", - "k=1;\n", - "l=1; #for plane (111)\n", - "\n", - "#Calculation\n", - "x=(2*m*e*V)**(1/2); \n", - "lamda=H/x; #wavelength(m)\n", - "d111=lamda*10**10/(2*math.sin(theta));\n", - "a=math.sqrt(h**2+k**2+l**2)*d111; #lattice parameter(angstrom)\n", - "\n", - "#Result\n", - "print \"lattice parameter is\",round(a,2),\"angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "lattice parameter is 2.59 angstrom\n" - ] - } - ], - "prompt_number": 49 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.12, Page number 224" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "epsilon0=8.85*10**-12;\n", - "r0=0.32*10**-9; #distance(m)\n", - "\n", - "#Calculation\n", - "V=-e/(4*math.pi*epsilon0*r0); #potential energy(eV)\n", - "\n", - "#Result\n", - "print \"potential energy is\",round(V,3),\"eV\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "potential energy is -4.496 eV\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 52 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.13, Page number 224" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "epsilon0=8.85*10**-12;\n", - "r0=0.31*10**-9; #distance(m)\n", - "n=9;\n", - "alpha=1.748; \n", - "Ie=5; #ionisation energy(eV)\n", - "ea=-3.61; #electron affinity(eV)\n", - "\n", - "#Calculation\n", - "a=1-(1/n);\n", - "Vr0=-alpha*e**2*a/(4*math.pi*epsilon0*r0); #energy(J)\n", - "Vr0=Vr0/e; #cohesive energy(eV)\n", - "Vr0i=Vr0/2; #contribution per ion to cohesive energy(eV)\n", - "Ee=Ie+ea; #electron transfer energy(eV)\n", - "Vr0i2=Ee/2; #contribution per ion to cohesive energy(eV)\n", - "CE=Vr0i+Vr0i2; #cohesive energy per atom(eV)\n", - "\n", - "#Result\n", - "print \"cohesive energy per atom is\",round(CE,4),\"eV\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "cohesive energy per atom is -2.9105 eV\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 58 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter10_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter10_1.ipynb deleted file mode 100755 index d4104917..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter10_1.ipynb +++ /dev/null @@ -1,434 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:de4c224e2d9bad9e810e24de23e4ee016e17fa0ec4d45805b35802744f1cd3b7" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "10: Crystal structure and bonding" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.5, Page number 213" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h1=1;\n", - "k1=0;\n", - "l1=0; #for (100) plane\n", - "h2=1;\n", - "k2=1;\n", - "l2=1; #for (111) plane\n", - "a=1; #assume\n", - "\n", - "#Calculation\n", - "d100=a/math.sqrt(h1**2+k1**2+l1**2); #spacing between (100) plane\n", - "d111=a/math.sqrt(h2**2+k2**2+l2**2); #spacing between (111) plane\n", - "\n", - "#Result\n", - "print \"spacing between (100) plane is\",d100,\"a\"\n", - "print \"spacing between (111) plane is\",round(d111,3),\"a\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "spacing between (100) plane is 1.0 a\n", - "spacing between (111) plane is 0.577 a\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.6, Page number 213" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "r=0.152; #atomic radius(nm)\n", - "h1=2;\n", - "k1=3;\n", - "l1=1; #for plane (231)\n", - "h2=1;\n", - "k2=1;\n", - "l2=0; #for plane (110)\n", - "\n", - "#Calculation\n", - "a=4*r/math.sqrt(2);\n", - "d231=a/math.sqrt(h1**2+k1**2+l1**2); #spacing between (231) plane(nm) \n", - "d110=a/math.sqrt(h2**2+k2**2+l2**2); #spacing between (110) plane(nm)\n", - "\n", - "#Result\n", - "print \"spacing between (231) plane is\",round(d231,4),\"nm\"\n", - "print \"spacing between (110) plane is\",d110,\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "spacing between (231) plane is 0.1149 nm\n", - "spacing between (110) plane is 0.304 nm\n" - ] - } - ], - "prompt_number": 4 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.7, Page number 213" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=1;\n", - "k=0;\n", - "l=2; #for plane (102)\n", - "a=0.424; #edge(nm)\n", - "\n", - "#Calculation\n", - "d102=a/math.sqrt(h**2+k**2+l**2); #interplanar spacing(nm)\n", - "\n", - "#Result\n", - "print \"interplanar spacing is\",round(d102,4),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "interplanar spacing is 0.1896 nm\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.8, Page number 214" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=3.2*10**-10; #edge(m)\n", - "rho=11.36*10**3; #density(kg/m**3)\n", - "N=6.023*10**26; #avagadro number(per k mol)\n", - "M=207.2; #atomic weight\n", - "\n", - "#Calculation\n", - "n=a**3*rho*N/M; #number of atoms per unit cell\n", - "\n", - "#Result\n", - "print \"number of atoms per unit cell is\",int(n)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number of atoms per unit cell is 1\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.9, Page number 220" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "d=2.51*10**-10; #spacing between planes(m)\n", - "theta=9; #glancing angle(degrees)\n", - "\n", - "#Calculation\n", - "theta=theta*math.pi/180; #glancing angle(radian)\n", - "lamda=2*d*math.sin(theta); #wavelength(m)\n", - "a=lamda/2.51;\n", - "theta2=math.asin(a); #glancing angle for 2nd order diffraction(radian)\n", - "theta2=2*theta*180/math.pi; #glancing angle for 2nd order diffraction(degrees)\n", - "\n", - "#Result\n", - "print \"wavelength of X ray is\",round(lamda*10**10,4),\"angstrom\"\n", - "print \"glancing angle for 2nd order diffraction is\",theta2,\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of X ray is 0.7853 angstrom\n", - "glancing angle for 2nd order diffraction is 18.0 degrees\n" - ] - } - ], - "prompt_number": 28 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.10, Page number 220" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=5*10**-10; #lattice parameter(m)\n", - "n=1;\n", - "lamda=1.4*10**-10; #wavelength(m)\n", - "h=1;\n", - "k=1;\n", - "l=1; #for plane (111)\n", - "\n", - "#Calculation\n", - "d111=a/math.sqrt(h**2+k**2+l**2);\n", - "b=n*lamda/(2*d111);\n", - "theta111=math.asin(b); #incident angle(radian)\n", - "theta111=theta111*180/math.pi; #incident angle(degrees)\n", - "\n", - "#Result\n", - "print \"incident angle is\",int(theta111),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "incident angle is 14 degrees\n" - ] - } - ], - "prompt_number": 30 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.11, Page number 221" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "H=6.626*10**-34; #planck's constant(Js)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "V=120; #potential(V)\n", - "theta=22; #angle(degrees)\n", - "theta=theta*math.pi/180; #angle(radian)\n", - "h=1;\n", - "k=1;\n", - "l=1; #for plane (111)\n", - "\n", - "#Calculation\n", - "x=(2*m*e*V)**(1/2); \n", - "lamda=H/x; #wavelength(m)\n", - "d111=lamda*10**10/(2*math.sin(theta));\n", - "a=math.sqrt(h**2+k**2+l**2)*d111; #lattice parameter(angstrom)\n", - "\n", - "#Result\n", - "print \"lattice parameter is\",round(a,2),\"angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "lattice parameter is 2.59 angstrom\n" - ] - } - ], - "prompt_number": 49 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.12, Page number 224" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "epsilon0=8.85*10**-12;\n", - "r0=0.32*10**-9; #distance(m)\n", - "\n", - "#Calculation\n", - "V=-e/(4*math.pi*epsilon0*r0); #potential energy(eV)\n", - "\n", - "#Result\n", - "print \"potential energy is\",round(V,3),\"eV\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "potential energy is -4.496 eV\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 52 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.13, Page number 224" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "epsilon0=8.85*10**-12;\n", - "r0=0.31*10**-9; #distance(m)\n", - "n=9;\n", - "alpha=1.748; \n", - "Ie=5; #ionisation energy(eV)\n", - "ea=-3.61; #electron affinity(eV)\n", - "\n", - "#Calculation\n", - "a=1-(1/n);\n", - "Vr0=-alpha*e**2*a/(4*math.pi*epsilon0*r0); #energy(J)\n", - "Vr0=Vr0/e; #cohesive energy(eV)\n", - "Vr0i=Vr0/2; #contribution per ion to cohesive energy(eV)\n", - "Ee=Ie+ea; #electron transfer energy(eV)\n", - "Vr0i2=Ee/2; #contribution per ion to cohesive energy(eV)\n", - "CE=Vr0i+Vr0i2; #cohesive energy per atom(eV)\n", - "\n", - "#Result\n", - "print \"cohesive energy per atom is\",round(CE,4),\"eV\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "cohesive energy per atom is -2.9105 eV\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 58 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter10_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter10_2.ipynb deleted file mode 100755 index d4104917..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter10_2.ipynb +++ /dev/null @@ -1,434 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:de4c224e2d9bad9e810e24de23e4ee016e17fa0ec4d45805b35802744f1cd3b7" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "10: Crystal structure and bonding" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.5, Page number 213" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h1=1;\n", - "k1=0;\n", - "l1=0; #for (100) plane\n", - "h2=1;\n", - "k2=1;\n", - "l2=1; #for (111) plane\n", - "a=1; #assume\n", - "\n", - "#Calculation\n", - "d100=a/math.sqrt(h1**2+k1**2+l1**2); #spacing between (100) plane\n", - "d111=a/math.sqrt(h2**2+k2**2+l2**2); #spacing between (111) plane\n", - "\n", - "#Result\n", - "print \"spacing between (100) plane is\",d100,\"a\"\n", - "print \"spacing between (111) plane is\",round(d111,3),\"a\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "spacing between (100) plane is 1.0 a\n", - "spacing between (111) plane is 0.577 a\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.6, Page number 213" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "r=0.152; #atomic radius(nm)\n", - "h1=2;\n", - "k1=3;\n", - "l1=1; #for plane (231)\n", - "h2=1;\n", - "k2=1;\n", - "l2=0; #for plane (110)\n", - "\n", - "#Calculation\n", - "a=4*r/math.sqrt(2);\n", - "d231=a/math.sqrt(h1**2+k1**2+l1**2); #spacing between (231) plane(nm) \n", - "d110=a/math.sqrt(h2**2+k2**2+l2**2); #spacing between (110) plane(nm)\n", - "\n", - "#Result\n", - "print \"spacing between (231) plane is\",round(d231,4),\"nm\"\n", - "print \"spacing between (110) plane is\",d110,\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "spacing between (231) plane is 0.1149 nm\n", - "spacing between (110) plane is 0.304 nm\n" - ] - } - ], - "prompt_number": 4 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.7, Page number 213" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=1;\n", - "k=0;\n", - "l=2; #for plane (102)\n", - "a=0.424; #edge(nm)\n", - "\n", - "#Calculation\n", - "d102=a/math.sqrt(h**2+k**2+l**2); #interplanar spacing(nm)\n", - "\n", - "#Result\n", - "print \"interplanar spacing is\",round(d102,4),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "interplanar spacing is 0.1896 nm\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.8, Page number 214" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=3.2*10**-10; #edge(m)\n", - "rho=11.36*10**3; #density(kg/m**3)\n", - "N=6.023*10**26; #avagadro number(per k mol)\n", - "M=207.2; #atomic weight\n", - "\n", - "#Calculation\n", - "n=a**3*rho*N/M; #number of atoms per unit cell\n", - "\n", - "#Result\n", - "print \"number of atoms per unit cell is\",int(n)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number of atoms per unit cell is 1\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.9, Page number 220" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "d=2.51*10**-10; #spacing between planes(m)\n", - "theta=9; #glancing angle(degrees)\n", - "\n", - "#Calculation\n", - "theta=theta*math.pi/180; #glancing angle(radian)\n", - "lamda=2*d*math.sin(theta); #wavelength(m)\n", - "a=lamda/2.51;\n", - "theta2=math.asin(a); #glancing angle for 2nd order diffraction(radian)\n", - "theta2=2*theta*180/math.pi; #glancing angle for 2nd order diffraction(degrees)\n", - "\n", - "#Result\n", - "print \"wavelength of X ray is\",round(lamda*10**10,4),\"angstrom\"\n", - "print \"glancing angle for 2nd order diffraction is\",theta2,\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of X ray is 0.7853 angstrom\n", - "glancing angle for 2nd order diffraction is 18.0 degrees\n" - ] - } - ], - "prompt_number": 28 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.10, Page number 220" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=5*10**-10; #lattice parameter(m)\n", - "n=1;\n", - "lamda=1.4*10**-10; #wavelength(m)\n", - "h=1;\n", - "k=1;\n", - "l=1; #for plane (111)\n", - "\n", - "#Calculation\n", - "d111=a/math.sqrt(h**2+k**2+l**2);\n", - "b=n*lamda/(2*d111);\n", - "theta111=math.asin(b); #incident angle(radian)\n", - "theta111=theta111*180/math.pi; #incident angle(degrees)\n", - "\n", - "#Result\n", - "print \"incident angle is\",int(theta111),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "incident angle is 14 degrees\n" - ] - } - ], - "prompt_number": 30 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.11, Page number 221" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "H=6.626*10**-34; #planck's constant(Js)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "V=120; #potential(V)\n", - "theta=22; #angle(degrees)\n", - "theta=theta*math.pi/180; #angle(radian)\n", - "h=1;\n", - "k=1;\n", - "l=1; #for plane (111)\n", - "\n", - "#Calculation\n", - "x=(2*m*e*V)**(1/2); \n", - "lamda=H/x; #wavelength(m)\n", - "d111=lamda*10**10/(2*math.sin(theta));\n", - "a=math.sqrt(h**2+k**2+l**2)*d111; #lattice parameter(angstrom)\n", - "\n", - "#Result\n", - "print \"lattice parameter is\",round(a,2),\"angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "lattice parameter is 2.59 angstrom\n" - ] - } - ], - "prompt_number": 49 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.12, Page number 224" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "epsilon0=8.85*10**-12;\n", - "r0=0.32*10**-9; #distance(m)\n", - "\n", - "#Calculation\n", - "V=-e/(4*math.pi*epsilon0*r0); #potential energy(eV)\n", - "\n", - "#Result\n", - "print \"potential energy is\",round(V,3),\"eV\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "potential energy is -4.496 eV\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 52 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 10.13, Page number 224" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "epsilon0=8.85*10**-12;\n", - "r0=0.31*10**-9; #distance(m)\n", - "n=9;\n", - "alpha=1.748; \n", - "Ie=5; #ionisation energy(eV)\n", - "ea=-3.61; #electron affinity(eV)\n", - "\n", - "#Calculation\n", - "a=1-(1/n);\n", - "Vr0=-alpha*e**2*a/(4*math.pi*epsilon0*r0); #energy(J)\n", - "Vr0=Vr0/e; #cohesive energy(eV)\n", - "Vr0i=Vr0/2; #contribution per ion to cohesive energy(eV)\n", - "Ee=Ie+ea; #electron transfer energy(eV)\n", - "Vr0i2=Ee/2; #contribution per ion to cohesive energy(eV)\n", - "CE=Vr0i+Vr0i2; #cohesive energy per atom(eV)\n", - "\n", - "#Result\n", - "print \"cohesive energy per atom is\",round(CE,4),\"eV\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "cohesive energy per atom is -2.9105 eV\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 58 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter11.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter11.ipynb deleted file mode 100755 index ffdec850..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter11.ipynb +++ /dev/null @@ -1,114 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:df9996e09d849b24524dd415b626cbe4279b4acdbe25d68bb407e2d42467c7a7" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "11: Lattice dynamics" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 11.1, Page number 238" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "thetaD=350; #temperature for Cu(K)\n", - "theetaD=550; #temperature for Si(K)\n", - "\n", - "#Calculation\n", - "newDCu=k*thetaD/h; #highest possible frequency for Cu(per sec)\n", - "newDSi=k*theetaD/h; #highest possible frequency for Si(per sec)\n", - "\n", - "#Result\n", - "print \"highest possible frequency for Cu is\",round(newDCu/10**11,3),\"*10**11 per sec\"\n", - "print \"highest possible frequency for Si is\",round(newDSi/10**11,2),\"*10**11 per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "highest possible frequency for Cu is 72.895 *10**11 per sec\n", - "highest possible frequency for Si is 114.55 *10**11 per sec\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 11.2, Page number 238" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "N=6.02*10**26; #avagadro number(k/mole)\n", - "T=10; #temperature(K)\n", - "thetaD=105; #debye temperature(K)\n", - "\n", - "#Calculation\n", - "C=(12/5)*(math.pi**4)*N*k*(T/thetaD)**3; #specific heat of lead(J/K kmol)\n", - "newD=k*thetaD/h; #highest frequency(per sec)\n", - "\n", - "#Result\n", - "print \"specific heat of lead is\",round(C,1),\"J/K kmol\"\n", - "print \"answer varies due to rounding off errors\"\n", - "print \"highest frequency is\",round(newD/10**11,2),\"*10**11 per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "specific heat of lead is 1677.7 J/K kmol\n", - "answer varies due to rounding off errors\n", - "highest frequency is 21.87 *10**11 per sec\n" - ] - } - ], - "prompt_number": 6 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter11_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter11_1.ipynb deleted file mode 100755 index ffdec850..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter11_1.ipynb +++ /dev/null @@ -1,114 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:df9996e09d849b24524dd415b626cbe4279b4acdbe25d68bb407e2d42467c7a7" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "11: Lattice dynamics" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 11.1, Page number 238" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "thetaD=350; #temperature for Cu(K)\n", - "theetaD=550; #temperature for Si(K)\n", - "\n", - "#Calculation\n", - "newDCu=k*thetaD/h; #highest possible frequency for Cu(per sec)\n", - "newDSi=k*theetaD/h; #highest possible frequency for Si(per sec)\n", - "\n", - "#Result\n", - "print \"highest possible frequency for Cu is\",round(newDCu/10**11,3),\"*10**11 per sec\"\n", - "print \"highest possible frequency for Si is\",round(newDSi/10**11,2),\"*10**11 per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "highest possible frequency for Cu is 72.895 *10**11 per sec\n", - "highest possible frequency for Si is 114.55 *10**11 per sec\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 11.2, Page number 238" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "N=6.02*10**26; #avagadro number(k/mole)\n", - "T=10; #temperature(K)\n", - "thetaD=105; #debye temperature(K)\n", - "\n", - "#Calculation\n", - "C=(12/5)*(math.pi**4)*N*k*(T/thetaD)**3; #specific heat of lead(J/K kmol)\n", - "newD=k*thetaD/h; #highest frequency(per sec)\n", - "\n", - "#Result\n", - "print \"specific heat of lead is\",round(C,1),\"J/K kmol\"\n", - "print \"answer varies due to rounding off errors\"\n", - "print \"highest frequency is\",round(newD/10**11,2),\"*10**11 per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "specific heat of lead is 1677.7 J/K kmol\n", - "answer varies due to rounding off errors\n", - "highest frequency is 21.87 *10**11 per sec\n" - ] - } - ], - "prompt_number": 6 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter11_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter11_2.ipynb deleted file mode 100755 index ffdec850..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter11_2.ipynb +++ /dev/null @@ -1,114 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:df9996e09d849b24524dd415b626cbe4279b4acdbe25d68bb407e2d42467c7a7" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "11: Lattice dynamics" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 11.1, Page number 238" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "thetaD=350; #temperature for Cu(K)\n", - "theetaD=550; #temperature for Si(K)\n", - "\n", - "#Calculation\n", - "newDCu=k*thetaD/h; #highest possible frequency for Cu(per sec)\n", - "newDSi=k*theetaD/h; #highest possible frequency for Si(per sec)\n", - "\n", - "#Result\n", - "print \"highest possible frequency for Cu is\",round(newDCu/10**11,3),\"*10**11 per sec\"\n", - "print \"highest possible frequency for Si is\",round(newDSi/10**11,2),\"*10**11 per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "highest possible frequency for Cu is 72.895 *10**11 per sec\n", - "highest possible frequency for Si is 114.55 *10**11 per sec\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 11.2, Page number 238" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "N=6.02*10**26; #avagadro number(k/mole)\n", - "T=10; #temperature(K)\n", - "thetaD=105; #debye temperature(K)\n", - "\n", - "#Calculation\n", - "C=(12/5)*(math.pi**4)*N*k*(T/thetaD)**3; #specific heat of lead(J/K kmol)\n", - "newD=k*thetaD/h; #highest frequency(per sec)\n", - "\n", - "#Result\n", - "print \"specific heat of lead is\",round(C,1),\"J/K kmol\"\n", - "print \"answer varies due to rounding off errors\"\n", - "print \"highest frequency is\",round(newD/10**11,2),\"*10**11 per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "specific heat of lead is 1677.7 J/K kmol\n", - "answer varies due to rounding off errors\n", - "highest frequency is 21.87 *10**11 per sec\n" - ] - } - ], - "prompt_number": 6 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter12.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter12.ipynb deleted file mode 100755 index b3818649..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter12.ipynb +++ /dev/null @@ -1,285 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:881432a5cd98267b92bdfa11e021925fdef61ae98abdadccafbf254c6f9ca038" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "12: Band theory of solids" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.1, Page number 243" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "EF=8; #fermi energy(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "E0bar=3*EF/5; \n", - "v=math.sqrt(2*E0bar*e/m); #speed of electron(m/s)\n", - "\n", - "#Result\n", - "print \"speed of electron is\",round(v/10**6,1),\"*10**6 m/s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of electron is 1.3 *10**6 m/s\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.2, Page number 244" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "I=8; #current(ampere)\n", - "r=9*10**-4; #radius(m)\n", - "V=5; #potential difference(V)\n", - "L=1; #length(m)\n", - "\n", - "#Calculation\n", - "A=math.pi*r**2; #area of wire(m**2)\n", - "E=V/L;\n", - "J=I/A; #current density(V/m)\n", - "rho=E/J; #resistivity(ohm m)\n", - "\n", - "#Result\n", - "print \"current density is\",round(J/10**6,3),\"*10**6 V/m\"\n", - "print \"resistivity is\",round(rho*10**6,2),\"*10**-6 ohm m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "current density is 3.144 *10**6 V/m\n", - "resistivity is 1.59 *10**-6 ohm m\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.3, Page number 245" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n=1;\n", - "a=4*10**-10; #lattice parameter(m)\n", - "N=1.56*10**28; \n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "tow=10**-15; #collision time(s)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "N=n/(a**3); #number of electrons per unit volume(per m**3)\n", - "sigma=N*e**2*tow/m; #conductivity(per ohm m)\n", - "rho=1/sigma; #resistivity(ohm m)\n", - "\n", - "#Result\n", - "print \"conductivity is\",round(sigma/10**6,2),\"*10**6 ohm m\"\n", - "print \"resistivity is\",rho,\"ohm m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "conductivity is 0.44 *10**6 ohm m\n", - "resistivity is 2.275e-06 ohm m\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.4, Page number 247" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "NA=6.02*10**26; #avagadro number(k/mole)\n", - "T=300; #temperature(K)\n", - "EF=2; #fermi energy(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "C=math.pi**2*k**2*NA*T/(2*EF*e); #electronic specific heat(J/kmol/K)\n", - "\n", - "#Result\n", - "print \"electronic specific heat is\",int(C),\"J/kmol/K\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "electronic specific heat is 530 J/kmol/K\n" - ] - } - ], - "prompt_number": 10 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.5, Page number 247" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "K=327; #thermal conductivity(W/mK)\n", - "T=300; #temperature(K)\n", - "rho=7.13*10**3; #density(kg/m**3)\n", - "NA=6.02*10**26; #avagadro number(k/mole)\n", - "w=65.38; #atomic weight\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "tow=2.5*10**-14; #relaxation time(s)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "N=2*rho*NA/w; #number of electrons per unit volume(per m**3)\n", - "sigma=N*e**2*tow/m; #conductivity(per ohm m)\n", - "L=K/(sigma*T); #lorentz number(W ohm/K**2)\n", - "\n", - "#Result\n", - "print \"lorentz number is\",round(L*10**8,4),\"*10**-8 W ohm/K**2\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "lorentz number is 1.1804 *10**-8 W ohm/K**2\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.6, Page number 248" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "n=5*10**28; #number of atoms(/m**3)\n", - "\n", - "#Calculation\n", - "RH=-1/(n*e); #hall coefficient(m**3/C)\n", - "\n", - "#Result\n", - "print \"hall coefficient is\",round(RH*10**9,3),\"*10**-9 m**3/C\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "hall coefficient is -0.125 *10**-9 m**3/C\n" - ] - } - ], - "prompt_number": 14 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter12_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter12_1.ipynb deleted file mode 100755 index b3818649..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter12_1.ipynb +++ /dev/null @@ -1,285 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:881432a5cd98267b92bdfa11e021925fdef61ae98abdadccafbf254c6f9ca038" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "12: Band theory of solids" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.1, Page number 243" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "EF=8; #fermi energy(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "E0bar=3*EF/5; \n", - "v=math.sqrt(2*E0bar*e/m); #speed of electron(m/s)\n", - "\n", - "#Result\n", - "print \"speed of electron is\",round(v/10**6,1),\"*10**6 m/s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of electron is 1.3 *10**6 m/s\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.2, Page number 244" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "I=8; #current(ampere)\n", - "r=9*10**-4; #radius(m)\n", - "V=5; #potential difference(V)\n", - "L=1; #length(m)\n", - "\n", - "#Calculation\n", - "A=math.pi*r**2; #area of wire(m**2)\n", - "E=V/L;\n", - "J=I/A; #current density(V/m)\n", - "rho=E/J; #resistivity(ohm m)\n", - "\n", - "#Result\n", - "print \"current density is\",round(J/10**6,3),\"*10**6 V/m\"\n", - "print \"resistivity is\",round(rho*10**6,2),\"*10**-6 ohm m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "current density is 3.144 *10**6 V/m\n", - "resistivity is 1.59 *10**-6 ohm m\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.3, Page number 245" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n=1;\n", - "a=4*10**-10; #lattice parameter(m)\n", - "N=1.56*10**28; \n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "tow=10**-15; #collision time(s)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "N=n/(a**3); #number of electrons per unit volume(per m**3)\n", - "sigma=N*e**2*tow/m; #conductivity(per ohm m)\n", - "rho=1/sigma; #resistivity(ohm m)\n", - "\n", - "#Result\n", - "print \"conductivity is\",round(sigma/10**6,2),\"*10**6 ohm m\"\n", - "print \"resistivity is\",rho,\"ohm m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "conductivity is 0.44 *10**6 ohm m\n", - "resistivity is 2.275e-06 ohm m\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.4, Page number 247" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "NA=6.02*10**26; #avagadro number(k/mole)\n", - "T=300; #temperature(K)\n", - "EF=2; #fermi energy(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "C=math.pi**2*k**2*NA*T/(2*EF*e); #electronic specific heat(J/kmol/K)\n", - "\n", - "#Result\n", - "print \"electronic specific heat is\",int(C),\"J/kmol/K\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "electronic specific heat is 530 J/kmol/K\n" - ] - } - ], - "prompt_number": 10 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.5, Page number 247" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "K=327; #thermal conductivity(W/mK)\n", - "T=300; #temperature(K)\n", - "rho=7.13*10**3; #density(kg/m**3)\n", - "NA=6.02*10**26; #avagadro number(k/mole)\n", - "w=65.38; #atomic weight\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "tow=2.5*10**-14; #relaxation time(s)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "N=2*rho*NA/w; #number of electrons per unit volume(per m**3)\n", - "sigma=N*e**2*tow/m; #conductivity(per ohm m)\n", - "L=K/(sigma*T); #lorentz number(W ohm/K**2)\n", - "\n", - "#Result\n", - "print \"lorentz number is\",round(L*10**8,4),\"*10**-8 W ohm/K**2\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "lorentz number is 1.1804 *10**-8 W ohm/K**2\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.6, Page number 248" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "n=5*10**28; #number of atoms(/m**3)\n", - "\n", - "#Calculation\n", - "RH=-1/(n*e); #hall coefficient(m**3/C)\n", - "\n", - "#Result\n", - "print \"hall coefficient is\",round(RH*10**9,3),\"*10**-9 m**3/C\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "hall coefficient is -0.125 *10**-9 m**3/C\n" - ] - } - ], - "prompt_number": 14 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter12_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter12_2.ipynb deleted file mode 100755 index b3818649..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter12_2.ipynb +++ /dev/null @@ -1,285 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:881432a5cd98267b92bdfa11e021925fdef61ae98abdadccafbf254c6f9ca038" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "12: Band theory of solids" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.1, Page number 243" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "EF=8; #fermi energy(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "E0bar=3*EF/5; \n", - "v=math.sqrt(2*E0bar*e/m); #speed of electron(m/s)\n", - "\n", - "#Result\n", - "print \"speed of electron is\",round(v/10**6,1),\"*10**6 m/s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of electron is 1.3 *10**6 m/s\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.2, Page number 244" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "I=8; #current(ampere)\n", - "r=9*10**-4; #radius(m)\n", - "V=5; #potential difference(V)\n", - "L=1; #length(m)\n", - "\n", - "#Calculation\n", - "A=math.pi*r**2; #area of wire(m**2)\n", - "E=V/L;\n", - "J=I/A; #current density(V/m)\n", - "rho=E/J; #resistivity(ohm m)\n", - "\n", - "#Result\n", - "print \"current density is\",round(J/10**6,3),\"*10**6 V/m\"\n", - "print \"resistivity is\",round(rho*10**6,2),\"*10**-6 ohm m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "current density is 3.144 *10**6 V/m\n", - "resistivity is 1.59 *10**-6 ohm m\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.3, Page number 245" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n=1;\n", - "a=4*10**-10; #lattice parameter(m)\n", - "N=1.56*10**28; \n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "tow=10**-15; #collision time(s)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "N=n/(a**3); #number of electrons per unit volume(per m**3)\n", - "sigma=N*e**2*tow/m; #conductivity(per ohm m)\n", - "rho=1/sigma; #resistivity(ohm m)\n", - "\n", - "#Result\n", - "print \"conductivity is\",round(sigma/10**6,2),\"*10**6 ohm m\"\n", - "print \"resistivity is\",rho,\"ohm m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "conductivity is 0.44 *10**6 ohm m\n", - "resistivity is 2.275e-06 ohm m\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.4, Page number 247" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "NA=6.02*10**26; #avagadro number(k/mole)\n", - "T=300; #temperature(K)\n", - "EF=2; #fermi energy(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "C=math.pi**2*k**2*NA*T/(2*EF*e); #electronic specific heat(J/kmol/K)\n", - "\n", - "#Result\n", - "print \"electronic specific heat is\",int(C),\"J/kmol/K\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "electronic specific heat is 530 J/kmol/K\n" - ] - } - ], - "prompt_number": 10 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.5, Page number 247" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "K=327; #thermal conductivity(W/mK)\n", - "T=300; #temperature(K)\n", - "rho=7.13*10**3; #density(kg/m**3)\n", - "NA=6.02*10**26; #avagadro number(k/mole)\n", - "w=65.38; #atomic weight\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "tow=2.5*10**-14; #relaxation time(s)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "N=2*rho*NA/w; #number of electrons per unit volume(per m**3)\n", - "sigma=N*e**2*tow/m; #conductivity(per ohm m)\n", - "L=K/(sigma*T); #lorentz number(W ohm/K**2)\n", - "\n", - "#Result\n", - "print \"lorentz number is\",round(L*10**8,4),\"*10**-8 W ohm/K**2\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "lorentz number is 1.1804 *10**-8 W ohm/K**2\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 12.6, Page number 248" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "n=5*10**28; #number of atoms(/m**3)\n", - "\n", - "#Calculation\n", - "RH=-1/(n*e); #hall coefficient(m**3/C)\n", - "\n", - "#Result\n", - "print \"hall coefficient is\",round(RH*10**9,3),\"*10**-9 m**3/C\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "hall coefficient is -0.125 *10**-9 m**3/C\n" - ] - } - ], - "prompt_number": 14 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter13.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter13.ipynb deleted file mode 100755 index 70f718e0..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter13.ipynb +++ /dev/null @@ -1,250 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:1e02413599230fcf3193c09944545ea5772a7d8e9a89055fec5a43dcb6e7435b" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "13: Magnetic properties of solids" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.1, Page number 256" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "chi=-4.2*10**-6; #magnetic susceptibility\n", - "H=1.2*10**5; #magnetic field(A/m)\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "\n", - "#Calculation\n", - "M=chi*H; #magnetisation(A/m)\n", - "B=mew0*(H+M); #flux density(T)\n", - "mewr=(M/H)+1; #relative permeability\n", - "\n", - "#Result\n", - "print \"magnetisation is\",M,\"A/m\"\n", - "print \"flux density is\",round(B,3),\"T\"\n", - "print \"relative permeability is\",round(mewr,6)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "magnetisation is -0.504 A/m\n", - "flux density is 0.151 T\n", - "relative permeability is 0.999996\n" - ] - } - ], - "prompt_number": 4 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.2, Page number 258" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "Z=2; #atomic number\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "N=28*10**26; #number of atoms(per m**3)\n", - "r=0.6*10**-10; #mean radius(m)\n", - "\n", - "#Calculation\n", - "chi=-mew0*Z*e**2*N*r**2/(6*m); #diamagnetic susceptibility\n", - "\n", - "#Result\n", - "print \"diamagnetic susceptibility is\",round(chi*10**8,3),\"*10**-8\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "diamagnetic susceptibility is -11.878 *10**-8\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.3, Page number 259" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n=2;\n", - "a=2.55*10**-10; #lattice constant(m)\n", - "chi=5.6*10**-6; #susceptibility\n", - "Z=1;\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "N=n/(a**3); #number of electrons per unit volume(per m**3)\n", - "rbar=math.sqrt(chi*6*m/(mew0*Z*e**2*N)); #radius of atom(m)\n", - "\n", - "#Result\n", - "print \"radius of atom is\",round(rbar*10**10,3),\"angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "radius of atom is 0.888 angstrom\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.4, Page number 260" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "T=300; #temperature(K)\n", - "N=6.5*10**25; #number of atoms(per m**3)\n", - "mew=9.27*10**-24; \n", - "\n", - "#Calculation\n", - "chi=mew0*N*mew**2/(3*k*T); #susceptibility\n", - "\n", - "#Result\n", - "print \"susceptibility is\",round(chi*10**7,2),\"*10**-7\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "susceptibility is 5.65 *10**-7\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.5, Page number 260" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "rho=4370; #density(kg/m**3)\n", - "NA=6.02*10**26; #avagadro number(k/mole)\n", - "M=168.5; #molecular weight(kg/kmol)\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "T=300; #temperature(K)\n", - "H=2*10**5; #electric field(A/m)\n", - "mew=2*9.27*10**-24; \n", - "\n", - "#Calculation\n", - "N=rho*NA/M; \n", - "chi=mew0*N*mew**2/(3*k*T); #susceptibility\n", - "M=chi*H; #magnetisation(A/m)\n", - "\n", - "#Result\n", - "print \"susceptibility is\",round(chi*10**4,4),\"*10**-4\"\n", - "print \"magnetisation is\",round(M,3),\"A/m\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "susceptibility is 5.4298 *10**-4\n", - "magnetisation is 108.596 A/m\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 17 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter13_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter13_1.ipynb deleted file mode 100755 index 70f718e0..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter13_1.ipynb +++ /dev/null @@ -1,250 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:1e02413599230fcf3193c09944545ea5772a7d8e9a89055fec5a43dcb6e7435b" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "13: Magnetic properties of solids" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.1, Page number 256" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "chi=-4.2*10**-6; #magnetic susceptibility\n", - "H=1.2*10**5; #magnetic field(A/m)\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "\n", - "#Calculation\n", - "M=chi*H; #magnetisation(A/m)\n", - "B=mew0*(H+M); #flux density(T)\n", - "mewr=(M/H)+1; #relative permeability\n", - "\n", - "#Result\n", - "print \"magnetisation is\",M,\"A/m\"\n", - "print \"flux density is\",round(B,3),\"T\"\n", - "print \"relative permeability is\",round(mewr,6)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "magnetisation is -0.504 A/m\n", - "flux density is 0.151 T\n", - "relative permeability is 0.999996\n" - ] - } - ], - "prompt_number": 4 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.2, Page number 258" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "Z=2; #atomic number\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "N=28*10**26; #number of atoms(per m**3)\n", - "r=0.6*10**-10; #mean radius(m)\n", - "\n", - "#Calculation\n", - "chi=-mew0*Z*e**2*N*r**2/(6*m); #diamagnetic susceptibility\n", - "\n", - "#Result\n", - "print \"diamagnetic susceptibility is\",round(chi*10**8,3),\"*10**-8\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "diamagnetic susceptibility is -11.878 *10**-8\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.3, Page number 259" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n=2;\n", - "a=2.55*10**-10; #lattice constant(m)\n", - "chi=5.6*10**-6; #susceptibility\n", - "Z=1;\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "N=n/(a**3); #number of electrons per unit volume(per m**3)\n", - "rbar=math.sqrt(chi*6*m/(mew0*Z*e**2*N)); #radius of atom(m)\n", - "\n", - "#Result\n", - "print \"radius of atom is\",round(rbar*10**10,3),\"angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "radius of atom is 0.888 angstrom\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.4, Page number 260" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "T=300; #temperature(K)\n", - "N=6.5*10**25; #number of atoms(per m**3)\n", - "mew=9.27*10**-24; \n", - "\n", - "#Calculation\n", - "chi=mew0*N*mew**2/(3*k*T); #susceptibility\n", - "\n", - "#Result\n", - "print \"susceptibility is\",round(chi*10**7,2),\"*10**-7\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "susceptibility is 5.65 *10**-7\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.5, Page number 260" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "rho=4370; #density(kg/m**3)\n", - "NA=6.02*10**26; #avagadro number(k/mole)\n", - "M=168.5; #molecular weight(kg/kmol)\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "T=300; #temperature(K)\n", - "H=2*10**5; #electric field(A/m)\n", - "mew=2*9.27*10**-24; \n", - "\n", - "#Calculation\n", - "N=rho*NA/M; \n", - "chi=mew0*N*mew**2/(3*k*T); #susceptibility\n", - "M=chi*H; #magnetisation(A/m)\n", - "\n", - "#Result\n", - "print \"susceptibility is\",round(chi*10**4,4),\"*10**-4\"\n", - "print \"magnetisation is\",round(M,3),\"A/m\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "susceptibility is 5.4298 *10**-4\n", - "magnetisation is 108.596 A/m\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 17 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter13_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter13_2.ipynb deleted file mode 100755 index 70f718e0..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter13_2.ipynb +++ /dev/null @@ -1,250 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:1e02413599230fcf3193c09944545ea5772a7d8e9a89055fec5a43dcb6e7435b" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "13: Magnetic properties of solids" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.1, Page number 256" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "chi=-4.2*10**-6; #magnetic susceptibility\n", - "H=1.2*10**5; #magnetic field(A/m)\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "\n", - "#Calculation\n", - "M=chi*H; #magnetisation(A/m)\n", - "B=mew0*(H+M); #flux density(T)\n", - "mewr=(M/H)+1; #relative permeability\n", - "\n", - "#Result\n", - "print \"magnetisation is\",M,\"A/m\"\n", - "print \"flux density is\",round(B,3),\"T\"\n", - "print \"relative permeability is\",round(mewr,6)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "magnetisation is -0.504 A/m\n", - "flux density is 0.151 T\n", - "relative permeability is 0.999996\n" - ] - } - ], - "prompt_number": 4 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.2, Page number 258" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "Z=2; #atomic number\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "N=28*10**26; #number of atoms(per m**3)\n", - "r=0.6*10**-10; #mean radius(m)\n", - "\n", - "#Calculation\n", - "chi=-mew0*Z*e**2*N*r**2/(6*m); #diamagnetic susceptibility\n", - "\n", - "#Result\n", - "print \"diamagnetic susceptibility is\",round(chi*10**8,3),\"*10**-8\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "diamagnetic susceptibility is -11.878 *10**-8\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.3, Page number 259" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n=2;\n", - "a=2.55*10**-10; #lattice constant(m)\n", - "chi=5.6*10**-6; #susceptibility\n", - "Z=1;\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "N=n/(a**3); #number of electrons per unit volume(per m**3)\n", - "rbar=math.sqrt(chi*6*m/(mew0*Z*e**2*N)); #radius of atom(m)\n", - "\n", - "#Result\n", - "print \"radius of atom is\",round(rbar*10**10,3),\"angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "radius of atom is 0.888 angstrom\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.4, Page number 260" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "T=300; #temperature(K)\n", - "N=6.5*10**25; #number of atoms(per m**3)\n", - "mew=9.27*10**-24; \n", - "\n", - "#Calculation\n", - "chi=mew0*N*mew**2/(3*k*T); #susceptibility\n", - "\n", - "#Result\n", - "print \"susceptibility is\",round(chi*10**7,2),\"*10**-7\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "susceptibility is 5.65 *10**-7\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 13.5, Page number 260" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "rho=4370; #density(kg/m**3)\n", - "NA=6.02*10**26; #avagadro number(k/mole)\n", - "M=168.5; #molecular weight(kg/kmol)\n", - "mew0=4*math.pi*10**-7; #permitivity of free space(H/m)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "T=300; #temperature(K)\n", - "H=2*10**5; #electric field(A/m)\n", - "mew=2*9.27*10**-24; \n", - "\n", - "#Calculation\n", - "N=rho*NA/M; \n", - "chi=mew0*N*mew**2/(3*k*T); #susceptibility\n", - "M=chi*H; #magnetisation(A/m)\n", - "\n", - "#Result\n", - "print \"susceptibility is\",round(chi*10**4,4),\"*10**-4\"\n", - "print \"magnetisation is\",round(M,3),\"A/m\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "susceptibility is 5.4298 *10**-4\n", - "magnetisation is 108.596 A/m\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 17 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter14.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter14.ipynb deleted file mode 100755 index b2beeab9..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter14.ipynb +++ /dev/null @@ -1,107 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:f383b09bed78232b6f6bef91df71b6fd8febd00a3f89287a33c756d53748eb03" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "14: Superconductivity" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 14.1, Page number 272" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "Bc0=0.0305; #critical field(T)\n", - "T=2; #temperature(K)\n", - "Tc=3.722; #critical temperature(K)\n", - "r=2*10**-3; #diameter(m)\n", - "mew0=4*math.pi*10**-7; #magnetic permeability\n", - "\n", - "#Calculation\n", - "BcT=Bc0*(1-(T/Tc)**2); #critical field(T)\n", - "Ic=2*math.pi*r*BcT/mew0; #current(A)\n", - "\n", - "#Result\n", - "print \"current is\",round(Ic,1),\"A\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "current is 216.9 A\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 14.2, Page number 274" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamda0=37; #london penetration depth(nm)\n", - "T=5.2; #temperature(K)\n", - "Tc=7.193; #critical temperature(K)\n", - "\n", - "#Calculation\n", - "a=1-(T/Tc)**4;\n", - "lamdaT=lamda0*(a**(-1/2)); #penetration depth of lead(nm)\n", - "\n", - "#Result\n", - "print \"penetration depth of lead is\",round(lamdaT,3),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "penetration depth of lead is 43.398 nm\n" - ] - } - ], - "prompt_number": 7 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter14_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter14_1.ipynb deleted file mode 100755 index b2beeab9..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter14_1.ipynb +++ /dev/null @@ -1,107 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:f383b09bed78232b6f6bef91df71b6fd8febd00a3f89287a33c756d53748eb03" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "14: Superconductivity" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 14.1, Page number 272" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "Bc0=0.0305; #critical field(T)\n", - "T=2; #temperature(K)\n", - "Tc=3.722; #critical temperature(K)\n", - "r=2*10**-3; #diameter(m)\n", - "mew0=4*math.pi*10**-7; #magnetic permeability\n", - "\n", - "#Calculation\n", - "BcT=Bc0*(1-(T/Tc)**2); #critical field(T)\n", - "Ic=2*math.pi*r*BcT/mew0; #current(A)\n", - "\n", - "#Result\n", - "print \"current is\",round(Ic,1),\"A\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "current is 216.9 A\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 14.2, Page number 274" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamda0=37; #london penetration depth(nm)\n", - "T=5.2; #temperature(K)\n", - "Tc=7.193; #critical temperature(K)\n", - "\n", - "#Calculation\n", - "a=1-(T/Tc)**4;\n", - "lamdaT=lamda0*(a**(-1/2)); #penetration depth of lead(nm)\n", - "\n", - "#Result\n", - "print \"penetration depth of lead is\",round(lamdaT,3),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "penetration depth of lead is 43.398 nm\n" - ] - } - ], - "prompt_number": 7 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter14_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter14_2.ipynb deleted file mode 100755 index b2beeab9..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter14_2.ipynb +++ /dev/null @@ -1,107 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:f383b09bed78232b6f6bef91df71b6fd8febd00a3f89287a33c756d53748eb03" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "14: Superconductivity" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 14.1, Page number 272" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "Bc0=0.0305; #critical field(T)\n", - "T=2; #temperature(K)\n", - "Tc=3.722; #critical temperature(K)\n", - "r=2*10**-3; #diameter(m)\n", - "mew0=4*math.pi*10**-7; #magnetic permeability\n", - "\n", - "#Calculation\n", - "BcT=Bc0*(1-(T/Tc)**2); #critical field(T)\n", - "Ic=2*math.pi*r*BcT/mew0; #current(A)\n", - "\n", - "#Result\n", - "print \"current is\",round(Ic,1),\"A\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "current is 216.9 A\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 14.2, Page number 274" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamda0=37; #london penetration depth(nm)\n", - "T=5.2; #temperature(K)\n", - "Tc=7.193; #critical temperature(K)\n", - "\n", - "#Calculation\n", - "a=1-(T/Tc)**4;\n", - "lamdaT=lamda0*(a**(-1/2)); #penetration depth of lead(nm)\n", - "\n", - "#Result\n", - "print \"penetration depth of lead is\",round(lamdaT,3),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "penetration depth of lead is 43.398 nm\n" - ] - } - ], - "prompt_number": 7 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter15.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter15.ipynb deleted file mode 100755 index 48af1473..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter15.ipynb +++ /dev/null @@ -1,203 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:ede2b0bb266c67744fbe14f69a09ec9b5592c13400e7d0bf2db5fa598ebe9db1" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "15: Lasers" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.1, Page number 283" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "T=1000; #temperature(K)\n", - "new1=7.5*10**14; \n", - "new2=4.3*10**14;\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "\n", - "#Calculation\n", - "kT=k*T;\n", - "#optical region extends from 4000 to 7000 angstrom\n", - "hnew=h*(new1-new2); \n", - "\n", - "#Result\n", - "print \"value of kT is\",kT,\"J\"\n", - "print \"value of hnew is\",hnew,\"J\"\n", - "print \"hnew>kT.therefore spontaneous transitions are dominant ones in optical region\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "value of kT is 1.38e-20 J\n", - "value of hnew is 2.12032e-19 J\n", - "hnew>kT.therefore spontaneous transitions are dominant ones in optical region\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.2, Page number 298" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "P=0.6; #power(watt)\n", - "T=30*10**-3; #time(s)\n", - "lamda=640*10**-9; #wavelength(m)\n", - "\n", - "#Calculation\n", - "E=P*T; #energy deposited(J)\n", - "n=E*lamda/(h*c); #number of photons in each pulse\n", - "\n", - "#Result\n", - "print \"energy deposited is\",E,\"J\"\n", - "print \"number of photons in each pulse is\",round(n/10**16,1),\"*10**16\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy deposited is 0.018 J\n", - "number of photons in each pulse is 5.8 *10**16\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.3, Page number 298" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamda=5000*10**-10; #wavelength(m)\n", - "f=0.2; #focal length(m)\n", - "a=0.009; #radius of aperture(m)\n", - "P=2.5*10**-3; #power(W)\n", - "\n", - "#Calculation\n", - "A=math.pi*lamda**2*f**2/a**2; #area of spot at focal plane(m**2)\n", - "I=P/A; #intensity at focus(W/m**2)\n", - "\n", - "#Result\n", - "print \"area of spot at focal plane is\",round(A*10**10,2),\"*10**-10 m**2\"\n", - "print \"intensity at focus is\",round(I/10**6,3),\"*10**6 W/m**2\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "area of spot at focal plane is 3.88 *10**-10 m**2\n", - "intensity at focus is 6.446 *10**6 W/m**2\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.4, Page number 298" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamda=693*10**-9; #wavelength(m)\n", - "D=3*10**-3; #diameter of mirror(m)\n", - "d=300*10**3; #distance from earth(m)\n", - "\n", - "#Calculation\n", - "delta_theta=1.22*lamda/D; #angular spread(rad)\n", - "a=delta_theta*d; #diameter of beam on satellite(m)\n", - "\n", - "#Result\n", - "print \"angular spread is\",round(delta_theta*10**4,2),\"*10**-4 rad\"\n", - "print \"diameter of beam on satellite is\",round(a,2),\"m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "angular spread is 2.82 *10**-4 rad\n", - "diameter of beam on satellite is 84.55 m\n" - ] - } - ], - "prompt_number": 15 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter15_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter15_1.ipynb deleted file mode 100755 index 48af1473..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter15_1.ipynb +++ /dev/null @@ -1,203 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:ede2b0bb266c67744fbe14f69a09ec9b5592c13400e7d0bf2db5fa598ebe9db1" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "15: Lasers" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.1, Page number 283" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "T=1000; #temperature(K)\n", - "new1=7.5*10**14; \n", - "new2=4.3*10**14;\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "\n", - "#Calculation\n", - "kT=k*T;\n", - "#optical region extends from 4000 to 7000 angstrom\n", - "hnew=h*(new1-new2); \n", - "\n", - "#Result\n", - "print \"value of kT is\",kT,\"J\"\n", - "print \"value of hnew is\",hnew,\"J\"\n", - "print \"hnew>kT.therefore spontaneous transitions are dominant ones in optical region\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "value of kT is 1.38e-20 J\n", - "value of hnew is 2.12032e-19 J\n", - "hnew>kT.therefore spontaneous transitions are dominant ones in optical region\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.2, Page number 298" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "P=0.6; #power(watt)\n", - "T=30*10**-3; #time(s)\n", - "lamda=640*10**-9; #wavelength(m)\n", - "\n", - "#Calculation\n", - "E=P*T; #energy deposited(J)\n", - "n=E*lamda/(h*c); #number of photons in each pulse\n", - "\n", - "#Result\n", - "print \"energy deposited is\",E,\"J\"\n", - "print \"number of photons in each pulse is\",round(n/10**16,1),\"*10**16\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy deposited is 0.018 J\n", - "number of photons in each pulse is 5.8 *10**16\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.3, Page number 298" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamda=5000*10**-10; #wavelength(m)\n", - "f=0.2; #focal length(m)\n", - "a=0.009; #radius of aperture(m)\n", - "P=2.5*10**-3; #power(W)\n", - "\n", - "#Calculation\n", - "A=math.pi*lamda**2*f**2/a**2; #area of spot at focal plane(m**2)\n", - "I=P/A; #intensity at focus(W/m**2)\n", - "\n", - "#Result\n", - "print \"area of spot at focal plane is\",round(A*10**10,2),\"*10**-10 m**2\"\n", - "print \"intensity at focus is\",round(I/10**6,3),\"*10**6 W/m**2\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "area of spot at focal plane is 3.88 *10**-10 m**2\n", - "intensity at focus is 6.446 *10**6 W/m**2\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.4, Page number 298" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamda=693*10**-9; #wavelength(m)\n", - "D=3*10**-3; #diameter of mirror(m)\n", - "d=300*10**3; #distance from earth(m)\n", - "\n", - "#Calculation\n", - "delta_theta=1.22*lamda/D; #angular spread(rad)\n", - "a=delta_theta*d; #diameter of beam on satellite(m)\n", - "\n", - "#Result\n", - "print \"angular spread is\",round(delta_theta*10**4,2),\"*10**-4 rad\"\n", - "print \"diameter of beam on satellite is\",round(a,2),\"m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "angular spread is 2.82 *10**-4 rad\n", - "diameter of beam on satellite is 84.55 m\n" - ] - } - ], - "prompt_number": 15 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter15_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter15_2.ipynb deleted file mode 100755 index 48af1473..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter15_2.ipynb +++ /dev/null @@ -1,203 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:ede2b0bb266c67744fbe14f69a09ec9b5592c13400e7d0bf2db5fa598ebe9db1" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "15: Lasers" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.1, Page number 283" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "T=1000; #temperature(K)\n", - "new1=7.5*10**14; \n", - "new2=4.3*10**14;\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "\n", - "#Calculation\n", - "kT=k*T;\n", - "#optical region extends from 4000 to 7000 angstrom\n", - "hnew=h*(new1-new2); \n", - "\n", - "#Result\n", - "print \"value of kT is\",kT,\"J\"\n", - "print \"value of hnew is\",hnew,\"J\"\n", - "print \"hnew>kT.therefore spontaneous transitions are dominant ones in optical region\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "value of kT is 1.38e-20 J\n", - "value of hnew is 2.12032e-19 J\n", - "hnew>kT.therefore spontaneous transitions are dominant ones in optical region\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.2, Page number 298" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "P=0.6; #power(watt)\n", - "T=30*10**-3; #time(s)\n", - "lamda=640*10**-9; #wavelength(m)\n", - "\n", - "#Calculation\n", - "E=P*T; #energy deposited(J)\n", - "n=E*lamda/(h*c); #number of photons in each pulse\n", - "\n", - "#Result\n", - "print \"energy deposited is\",E,\"J\"\n", - "print \"number of photons in each pulse is\",round(n/10**16,1),\"*10**16\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy deposited is 0.018 J\n", - "number of photons in each pulse is 5.8 *10**16\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.3, Page number 298" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamda=5000*10**-10; #wavelength(m)\n", - "f=0.2; #focal length(m)\n", - "a=0.009; #radius of aperture(m)\n", - "P=2.5*10**-3; #power(W)\n", - "\n", - "#Calculation\n", - "A=math.pi*lamda**2*f**2/a**2; #area of spot at focal plane(m**2)\n", - "I=P/A; #intensity at focus(W/m**2)\n", - "\n", - "#Result\n", - "print \"area of spot at focal plane is\",round(A*10**10,2),\"*10**-10 m**2\"\n", - "print \"intensity at focus is\",round(I/10**6,3),\"*10**6 W/m**2\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "area of spot at focal plane is 3.88 *10**-10 m**2\n", - "intensity at focus is 6.446 *10**6 W/m**2\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 15.4, Page number 298" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamda=693*10**-9; #wavelength(m)\n", - "D=3*10**-3; #diameter of mirror(m)\n", - "d=300*10**3; #distance from earth(m)\n", - "\n", - "#Calculation\n", - "delta_theta=1.22*lamda/D; #angular spread(rad)\n", - "a=delta_theta*d; #diameter of beam on satellite(m)\n", - "\n", - "#Result\n", - "print \"angular spread is\",round(delta_theta*10**4,2),\"*10**-4 rad\"\n", - "print \"diameter of beam on satellite is\",round(a,2),\"m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "angular spread is 2.82 *10**-4 rad\n", - "diameter of beam on satellite is 84.55 m\n" - ] - } - ], - "prompt_number": 15 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter16.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter16.ipynb deleted file mode 100755 index 932f4802..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter16.ipynb +++ /dev/null @@ -1,114 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:8689775b6694dc6c6ea95bc809bbd7280d9553003ec1dbe78844db2dc6fa68f3" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "16: Fibre optics and holography" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 16.1, Page number 306" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n2=1.4; #refractive index of cladding\n", - "n1=1.43; #refractive index of core\n", - "\n", - "#Calculation\n", - "costhetac=n2/n1; \n", - "thetac=math.acos(costhetac); #propagation angle(radian)\n", - "thetac=thetac*180/math.pi; #propagation angle(degrees)\n", - "NA=math.sqrt(n1**2-n2**2); #numerical aperture\n", - "thetaa=math.asin(NA); #angle(radian)\n", - "thetaa=thetaa*180/math.pi; #angle(degrees)\n", - "thetaa=2*thetaa; #acceptance angle(degrees)\n", - "\n", - "#Result\n", - "print \"propagation angle is\",round(thetac,1),\"degrees\"\n", - "print \"numerical aperture is\",round(NA,4)\n", - "print \"acceptance angle is\",round(thetaa,2),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "propagation angle is 11.8 degrees\n", - "numerical aperture is 0.2914\n", - "acceptance angle is 33.88 degrees\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 16.3, Page number 311" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "z=30; #length of optical fibre(km)\n", - "alpha=0.8; #fibre loss(dB/km)\n", - "Pi=200; #input power(micro W)\n", - "\n", - "#Calculation\n", - "a=alpha*z/10;\n", - "b=10**a;\n", - "P0=Pi/b; #output power(micro W)\n", - "\n", - "#Result\n", - "print \"output power is\",round(P0,3),\"micro W\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "output power is 0.796 micro W\n" - ] - } - ], - "prompt_number": 10 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter16_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter16_1.ipynb deleted file mode 100755 index 932f4802..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter16_1.ipynb +++ /dev/null @@ -1,114 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:8689775b6694dc6c6ea95bc809bbd7280d9553003ec1dbe78844db2dc6fa68f3" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "16: Fibre optics and holography" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 16.1, Page number 306" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n2=1.4; #refractive index of cladding\n", - "n1=1.43; #refractive index of core\n", - "\n", - "#Calculation\n", - "costhetac=n2/n1; \n", - "thetac=math.acos(costhetac); #propagation angle(radian)\n", - "thetac=thetac*180/math.pi; #propagation angle(degrees)\n", - "NA=math.sqrt(n1**2-n2**2); #numerical aperture\n", - "thetaa=math.asin(NA); #angle(radian)\n", - "thetaa=thetaa*180/math.pi; #angle(degrees)\n", - "thetaa=2*thetaa; #acceptance angle(degrees)\n", - "\n", - "#Result\n", - "print \"propagation angle is\",round(thetac,1),\"degrees\"\n", - "print \"numerical aperture is\",round(NA,4)\n", - "print \"acceptance angle is\",round(thetaa,2),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "propagation angle is 11.8 degrees\n", - "numerical aperture is 0.2914\n", - "acceptance angle is 33.88 degrees\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 16.3, Page number 311" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "z=30; #length of optical fibre(km)\n", - "alpha=0.8; #fibre loss(dB/km)\n", - "Pi=200; #input power(micro W)\n", - "\n", - "#Calculation\n", - "a=alpha*z/10;\n", - "b=10**a;\n", - "P0=Pi/b; #output power(micro W)\n", - "\n", - "#Result\n", - "print \"output power is\",round(P0,3),\"micro W\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "output power is 0.796 micro W\n" - ] - } - ], - "prompt_number": 10 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter16_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter16_2.ipynb deleted file mode 100755 index 932f4802..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter16_2.ipynb +++ /dev/null @@ -1,114 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:8689775b6694dc6c6ea95bc809bbd7280d9553003ec1dbe78844db2dc6fa68f3" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "16: Fibre optics and holography" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 16.1, Page number 306" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n2=1.4; #refractive index of cladding\n", - "n1=1.43; #refractive index of core\n", - "\n", - "#Calculation\n", - "costhetac=n2/n1; \n", - "thetac=math.acos(costhetac); #propagation angle(radian)\n", - "thetac=thetac*180/math.pi; #propagation angle(degrees)\n", - "NA=math.sqrt(n1**2-n2**2); #numerical aperture\n", - "thetaa=math.asin(NA); #angle(radian)\n", - "thetaa=thetaa*180/math.pi; #angle(degrees)\n", - "thetaa=2*thetaa; #acceptance angle(degrees)\n", - "\n", - "#Result\n", - "print \"propagation angle is\",round(thetac,1),\"degrees\"\n", - "print \"numerical aperture is\",round(NA,4)\n", - "print \"acceptance angle is\",round(thetaa,2),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "propagation angle is 11.8 degrees\n", - "numerical aperture is 0.2914\n", - "acceptance angle is 33.88 degrees\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 16.3, Page number 311" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "z=30; #length of optical fibre(km)\n", - "alpha=0.8; #fibre loss(dB/km)\n", - "Pi=200; #input power(micro W)\n", - "\n", - "#Calculation\n", - "a=alpha*z/10;\n", - "b=10**a;\n", - "P0=Pi/b; #output power(micro W)\n", - "\n", - "#Result\n", - "print \"output power is\",round(P0,3),\"micro W\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "output power is 0.796 micro W\n" - ] - } - ], - "prompt_number": 10 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter17.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter17.ipynb deleted file mode 100755 index 61dae782..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter17.ipynb +++ /dev/null @@ -1,293 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:d405bf204e77196ade310e0be88ebb97609af7dc21d3bd3e418e5c80ec00e4d3" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "17: Nuclear properties" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.1, Page number 324" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m=1.67*10**-27; #nucleon mass(kg)\n", - "R0=1.2*10**-15; #radius of nucleus(m)\n", - "\n", - "#Calculation\n", - "d=m*3/(4*math.pi*R0**3); #density of nucleus(kg/m**3)\n", - "\n", - "#Result\n", - "print \"density of nucleus is\",round(d/10**17,1),\"*10**17 kg/m**3\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "density of nucleus is 2.3 *10**17 kg/m**3\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.2, Page number 324" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=1.2*10**-15;\n", - "k=9*10**9; #value of N(Nm**2/C**2)\n", - "q1=2;\n", - "q2=90;\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "r=a*((4**(1/3))+(228**(1/3))); #distance(m)\n", - "E=k*q1*q2*e**2/r; #kinetic energy(J)\n", - "E=E/(e*10**6); #kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"potential energy is 0. kinetic energy is\",round(E,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "potential energy is 0. kinetic energy is 28.1 MeV\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.3, Page number 326" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "E=2.48*10**4; #electric field(V/m)\n", - "m=1.6605*10**-27; #nucleon mass(kg)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "B=0.75; #magnetic field(T)\n", - "\n", - "#Calculation\n", - "r1=E*12*m/(e*B**2); #distance on photographic plate for 12C(m)\n", - "r1=r1*10**3; #distance on photographic plate for 12C(mm)\n", - "r2=E*13*m/(e*B**2); #distance on photographic plate for 13C(m)\n", - "r2=r2*10**3; #distance on photographic plate for 13C(mm)\n", - "r3=E*14*m/(e*B**2); #distance on photographic plate for 14C(m)\n", - "r3=r3*10**3; #distance on photographic plate for 14C(mm)\n", - "r4=(2*r2)-(2*r1); #distance between lines of 13C and 12C(mm)\n", - "r5=(2*r3)-(2*r2); #distance between lines of 14C and 13C(mm)\n", - "r=r4/2; #distance if ions are doubly charged(mm)\n", - "\n", - "#Result\n", - "print \"distance on photographic plate for 12C is\",round(r1,2),\"mm\"\n", - "print \"distance on photographic plate for 13C is\",round(r2,2),\"mm\"\n", - "print \"distance on photographic plate for 14C is\",round(r3,2),\"mm\"\n", - "print \"distance if ions are doubly charged is\",round(r,2),\"mm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "distance on photographic plate for 12C is 5.49 mm\n", - "distance on photographic plate for 13C is 5.95 mm\n", - "distance on photographic plate for 14C is 6.41 mm\n", - "distance if ions are doubly charged is 0.46 mm\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.4, Page number 327" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n=6; #number of neutrons\n", - "p=6; #number of protons\n", - "M=12; #mass of 12C6(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "mn=n*1.008665; #mass of neutrons(u)\n", - "mp=p*1.007825; #mass of hydrogen atoms(u)\n", - "m=mp+mn; #total mass(u)\n", - "md=m-M; #mass deficiency(u)\n", - "BE=md*E; #binding energy(MeV)\n", - "be=BE/12; #average binding energy per nucleon(MeV)\n", - "\n", - "#Result\n", - "print \"binding energy is\",round(BE,2),\"MeV\"\n", - "print \"average binding energy per nucleon is\",round(be,2),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "binding energy is 92.16 MeV\n", - "average binding energy per nucleon is 7.68 MeV\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.6, Page number 335" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "M22Na=21.9944; #mass of 22Na(u)\n", - "m=1.008665; #mass of last neutron(u)\n", - "M23Na=22.989767; #mass of 23Na(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "M=M22Na+m; \n", - "md=M-M23Na; #mass deficiency(u)\n", - "BE=md*E; #binding energy(MeV)\n", - "\n", - "#Result\n", - "print \"binding energy is\",round(BE,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "binding energy is 12.4 MeV\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.7, Page number 341" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "hbar=1.05*10**-34; \n", - "c=3*10**8; #speed of light(m/s)\n", - "mpi=140; #mass of pi-meson(MeV/c**2)\n", - "e=1.6*10**-13;\n", - "\n", - "#Calculation\n", - "r=hbar*c/(mpi*e); #range of nuclear force(m)\n", - "\n", - "#Result\n", - "print \"range of nuclear force is\",round(r*10**15,1),\"fm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "range of nuclear force is 1.4 fm\n" - ] - } - ], - "prompt_number": 13 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter17_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter17_1.ipynb deleted file mode 100755 index 61dae782..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter17_1.ipynb +++ /dev/null @@ -1,293 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:d405bf204e77196ade310e0be88ebb97609af7dc21d3bd3e418e5c80ec00e4d3" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "17: Nuclear properties" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.1, Page number 324" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m=1.67*10**-27; #nucleon mass(kg)\n", - "R0=1.2*10**-15; #radius of nucleus(m)\n", - "\n", - "#Calculation\n", - "d=m*3/(4*math.pi*R0**3); #density of nucleus(kg/m**3)\n", - "\n", - "#Result\n", - "print \"density of nucleus is\",round(d/10**17,1),\"*10**17 kg/m**3\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "density of nucleus is 2.3 *10**17 kg/m**3\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.2, Page number 324" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=1.2*10**-15;\n", - "k=9*10**9; #value of N(Nm**2/C**2)\n", - "q1=2;\n", - "q2=90;\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "r=a*((4**(1/3))+(228**(1/3))); #distance(m)\n", - "E=k*q1*q2*e**2/r; #kinetic energy(J)\n", - "E=E/(e*10**6); #kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"potential energy is 0. kinetic energy is\",round(E,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "potential energy is 0. kinetic energy is 28.1 MeV\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.3, Page number 326" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "E=2.48*10**4; #electric field(V/m)\n", - "m=1.6605*10**-27; #nucleon mass(kg)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "B=0.75; #magnetic field(T)\n", - "\n", - "#Calculation\n", - "r1=E*12*m/(e*B**2); #distance on photographic plate for 12C(m)\n", - "r1=r1*10**3; #distance on photographic plate for 12C(mm)\n", - "r2=E*13*m/(e*B**2); #distance on photographic plate for 13C(m)\n", - "r2=r2*10**3; #distance on photographic plate for 13C(mm)\n", - "r3=E*14*m/(e*B**2); #distance on photographic plate for 14C(m)\n", - "r3=r3*10**3; #distance on photographic plate for 14C(mm)\n", - "r4=(2*r2)-(2*r1); #distance between lines of 13C and 12C(mm)\n", - "r5=(2*r3)-(2*r2); #distance between lines of 14C and 13C(mm)\n", - "r=r4/2; #distance if ions are doubly charged(mm)\n", - "\n", - "#Result\n", - "print \"distance on photographic plate for 12C is\",round(r1,2),\"mm\"\n", - "print \"distance on photographic plate for 13C is\",round(r2,2),\"mm\"\n", - "print \"distance on photographic plate for 14C is\",round(r3,2),\"mm\"\n", - "print \"distance if ions are doubly charged is\",round(r,2),\"mm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "distance on photographic plate for 12C is 5.49 mm\n", - "distance on photographic plate for 13C is 5.95 mm\n", - "distance on photographic plate for 14C is 6.41 mm\n", - "distance if ions are doubly charged is 0.46 mm\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.4, Page number 327" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n=6; #number of neutrons\n", - "p=6; #number of protons\n", - "M=12; #mass of 12C6(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "mn=n*1.008665; #mass of neutrons(u)\n", - "mp=p*1.007825; #mass of hydrogen atoms(u)\n", - "m=mp+mn; #total mass(u)\n", - "md=m-M; #mass deficiency(u)\n", - "BE=md*E; #binding energy(MeV)\n", - "be=BE/12; #average binding energy per nucleon(MeV)\n", - "\n", - "#Result\n", - "print \"binding energy is\",round(BE,2),\"MeV\"\n", - "print \"average binding energy per nucleon is\",round(be,2),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "binding energy is 92.16 MeV\n", - "average binding energy per nucleon is 7.68 MeV\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.6, Page number 335" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "M22Na=21.9944; #mass of 22Na(u)\n", - "m=1.008665; #mass of last neutron(u)\n", - "M23Na=22.989767; #mass of 23Na(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "M=M22Na+m; \n", - "md=M-M23Na; #mass deficiency(u)\n", - "BE=md*E; #binding energy(MeV)\n", - "\n", - "#Result\n", - "print \"binding energy is\",round(BE,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "binding energy is 12.4 MeV\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.7, Page number 341" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "hbar=1.05*10**-34; \n", - "c=3*10**8; #speed of light(m/s)\n", - "mpi=140; #mass of pi-meson(MeV/c**2)\n", - "e=1.6*10**-13;\n", - "\n", - "#Calculation\n", - "r=hbar*c/(mpi*e); #range of nuclear force(m)\n", - "\n", - "#Result\n", - "print \"range of nuclear force is\",round(r*10**15,1),\"fm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "range of nuclear force is 1.4 fm\n" - ] - } - ], - "prompt_number": 13 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter17_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter17_2.ipynb deleted file mode 100755 index 61dae782..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter17_2.ipynb +++ /dev/null @@ -1,293 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:d405bf204e77196ade310e0be88ebb97609af7dc21d3bd3e418e5c80ec00e4d3" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "17: Nuclear properties" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.1, Page number 324" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m=1.67*10**-27; #nucleon mass(kg)\n", - "R0=1.2*10**-15; #radius of nucleus(m)\n", - "\n", - "#Calculation\n", - "d=m*3/(4*math.pi*R0**3); #density of nucleus(kg/m**3)\n", - "\n", - "#Result\n", - "print \"density of nucleus is\",round(d/10**17,1),\"*10**17 kg/m**3\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "density of nucleus is 2.3 *10**17 kg/m**3\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.2, Page number 324" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=1.2*10**-15;\n", - "k=9*10**9; #value of N(Nm**2/C**2)\n", - "q1=2;\n", - "q2=90;\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "r=a*((4**(1/3))+(228**(1/3))); #distance(m)\n", - "E=k*q1*q2*e**2/r; #kinetic energy(J)\n", - "E=E/(e*10**6); #kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"potential energy is 0. kinetic energy is\",round(E,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "potential energy is 0. kinetic energy is 28.1 MeV\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.3, Page number 326" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "E=2.48*10**4; #electric field(V/m)\n", - "m=1.6605*10**-27; #nucleon mass(kg)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "B=0.75; #magnetic field(T)\n", - "\n", - "#Calculation\n", - "r1=E*12*m/(e*B**2); #distance on photographic plate for 12C(m)\n", - "r1=r1*10**3; #distance on photographic plate for 12C(mm)\n", - "r2=E*13*m/(e*B**2); #distance on photographic plate for 13C(m)\n", - "r2=r2*10**3; #distance on photographic plate for 13C(mm)\n", - "r3=E*14*m/(e*B**2); #distance on photographic plate for 14C(m)\n", - "r3=r3*10**3; #distance on photographic plate for 14C(mm)\n", - "r4=(2*r2)-(2*r1); #distance between lines of 13C and 12C(mm)\n", - "r5=(2*r3)-(2*r2); #distance between lines of 14C and 13C(mm)\n", - "r=r4/2; #distance if ions are doubly charged(mm)\n", - "\n", - "#Result\n", - "print \"distance on photographic plate for 12C is\",round(r1,2),\"mm\"\n", - "print \"distance on photographic plate for 13C is\",round(r2,2),\"mm\"\n", - "print \"distance on photographic plate for 14C is\",round(r3,2),\"mm\"\n", - "print \"distance if ions are doubly charged is\",round(r,2),\"mm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "distance on photographic plate for 12C is 5.49 mm\n", - "distance on photographic plate for 13C is 5.95 mm\n", - "distance on photographic plate for 14C is 6.41 mm\n", - "distance if ions are doubly charged is 0.46 mm\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.4, Page number 327" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "n=6; #number of neutrons\n", - "p=6; #number of protons\n", - "M=12; #mass of 12C6(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "mn=n*1.008665; #mass of neutrons(u)\n", - "mp=p*1.007825; #mass of hydrogen atoms(u)\n", - "m=mp+mn; #total mass(u)\n", - "md=m-M; #mass deficiency(u)\n", - "BE=md*E; #binding energy(MeV)\n", - "be=BE/12; #average binding energy per nucleon(MeV)\n", - "\n", - "#Result\n", - "print \"binding energy is\",round(BE,2),\"MeV\"\n", - "print \"average binding energy per nucleon is\",round(be,2),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "binding energy is 92.16 MeV\n", - "average binding energy per nucleon is 7.68 MeV\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.6, Page number 335" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "M22Na=21.9944; #mass of 22Na(u)\n", - "m=1.008665; #mass of last neutron(u)\n", - "M23Na=22.989767; #mass of 23Na(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "M=M22Na+m; \n", - "md=M-M23Na; #mass deficiency(u)\n", - "BE=md*E; #binding energy(MeV)\n", - "\n", - "#Result\n", - "print \"binding energy is\",round(BE,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "binding energy is 12.4 MeV\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 17.7, Page number 341" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "hbar=1.05*10**-34; \n", - "c=3*10**8; #speed of light(m/s)\n", - "mpi=140; #mass of pi-meson(MeV/c**2)\n", - "e=1.6*10**-13;\n", - "\n", - "#Calculation\n", - "r=hbar*c/(mpi*e); #range of nuclear force(m)\n", - "\n", - "#Result\n", - "print \"range of nuclear force is\",round(r*10**15,1),\"fm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "range of nuclear force is 1.4 fm\n" - ] - } - ], - "prompt_number": 13 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter18.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter18.ipynb deleted file mode 100755 index b99ff137..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter18.ipynb +++ /dev/null @@ -1,366 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:0f6dea1f19194326599a9bca2989e912ed17e32f1ffb8d9305e16c13f8cacf2c" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "18: Radioactive decay" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.1, Page number 347" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "N0=1; #assume\n", - "\n", - "#Calculation\n", - "f=(N0/2)/N0; #fraction after t1/2\n", - "f1=(N0/4)/N0; #fraction after 2 half lives\n", - "f2=(N0/(2**5))/N0; #fraction after 5 half lives\n", - "f3=(N0/(2**10))/N0; #fraction after 10 half lives\n", - "\n", - "#Result\n", - "print \"fraction after 2 half lives is\",f1\n", - "print \"fraction after 5 half lives is\",f2\n", - "print \"fraction after 10 half lives is\",f3" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "fraction after 2 half lives is 0.25\n", - "fraction after 5 half lives is 0.03125\n", - "fraction after 10 half lives is 0.0009765625\n" - ] - } - ], - "prompt_number": 1 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.2, Page number 348" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "thalf=2.7*24*60*60; #half life(s)\n", - "m=1*10**-6; #mass(gm)\n", - "Na=6.02*10**23; #avagadro number(atoms/mol)\n", - "M=198; #molar mass(g/mol)\n", - "t=8*24*60*60;\n", - "\n", - "#Calculation\n", - "lamda=0.693/thalf; #decay constant(per sec)\n", - "N=m*Na/M; #number of nuclei(atoms)\n", - "A0=lamda*N; #activity(disintegrations per sec)\n", - "A=A0*math.exp(-lamda*t); #activity for 8 days(decays per sec)\n", - "\n", - "#Result\n", - "print \"decay constant is\",round(lamda*10**6,2),\"*10**-6 per sec\"\n", - "print \"activity is\",round(A0/10**9,2),\"*10**9 disintegrations per sec\"\n", - "print \"activity for 8 days is\",round(A/10**9,2),\"*10**9 decays per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "decay constant is 2.97 *10**-6 per sec\n", - "activity is 9.03 *10**9 disintegrations per sec\n", - "activity for 8 days is 1.16 *10**9 decays per sec\n" - ] - } - ], - "prompt_number": 10 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.3, Page number 348" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "thalf=5570*365*24*60*60; #half life(s)\n", - "dNbydt=3.7*10**10*2*10**-3; #number of decays per sec\n", - "m=14;\n", - "Na=6.02*10**23; #avagadro number(atoms/mol)\n", - "\n", - "#Calculation\n", - "lamda=0.693/thalf; #decay constant(per sec)\n", - "N=dNbydt/lamda; #number of atoms\n", - "mN=m*N/Na; #mass of 2mCi(g)\n", - "\n", - "#Result\n", - "print \"mass of 2mCi is\",round(mN*10**4,2),\"*10**-4 g\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "mass of 2mCi is 4.36 *10**-4 g\n" - ] - } - ], - "prompt_number": 23 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.5, Page number 353" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "thalf=1.25*10**9; #half life(yr)\n", - "r=10.2; #ratio of number of atoms\n", - "\n", - "#Calculation\n", - "a=1+r;\n", - "lamda=0.693/thalf; #decay constant(per yr)\n", - "t=math.log(a)/lamda; #time(yr)\n", - "\n", - "#Result\n", - "print \"the rock is\",round(t/10**9,2),\"*10**9 yrs old\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "the rock is 4.36 *10**9 yrs old\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.6, Page number 356" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mU=232.037131; #atomic mass of U(u)\n", - "mHe=4.002603; #atomic mass of He(u)\n", - "E=931.5; #energy(MeV)\n", - "KE=5.32; #kinetic energy of alpha particle(MeV)\n", - "\n", - "#Calculation\n", - "mTh=mU-mHe-(KE/E); #atomic mass of Th(u)\n", - "\n", - "#Result\n", - "print \"atomic mass of Th is\",round(mTh,5),\"u\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "atomic mass of Th is 228.02882 u\n" - ] - } - ], - "prompt_number": 14 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.7, Page number 359" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "E=931.5; #energy(MeV)\n", - "mX=11.011433; #mass of 11C(u)\n", - "mXdash=11.009305; #mass of 11B(u)\n", - "me=0.511;\n", - "\n", - "#Calculation\n", - "Q=(E*(mX-mXdash))-(2*me); #Q value for decay(MeV)\n", - "\n", - "#Result\n", - "print \"maximum energy is\",round(Q,2),\"MeV.minimum energy is zero\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "maximum energy is 0.96 MeV.minimum energy is zero\n" - ] - } - ], - "prompt_number": 16 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.8, Page number 359" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mK=39.963999; #mass of K(u)\n", - "mAr=39.962384; #mass of Ar(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "Q=(mK-mAr)*E; #kinetic energy of neutrino(MeV)\n", - "\n", - "#Result\n", - "print \"kinetic energy of neutrino is\",round(Q,3),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "kinetic energy of neutrino is 1.504 MeV\n" - ] - } - ], - "prompt_number": 18 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.9, Page number 360" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mN=12.018613; #mass of N(u)\n", - "mC=12; #mass of C(u)\n", - "me=0.000549; #mass of me(u)\n", - "E=931.5; #energy(MeV)\n", - "Egamma=4.43; #energy of emitted gamma ray(MeV)\n", - "\n", - "#Calculation\n", - "Q=(mN-mC-(2*me))*E; #Q value(MeV)\n", - "Emax=Q-Egamma; #maximum kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"maximum kinetic energy is\",round(Emax,2),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "maximum kinetic energy is 11.89 MeV\n" - ] - } - ], - "prompt_number": 20 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter18_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter18_1.ipynb deleted file mode 100755 index b99ff137..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter18_1.ipynb +++ /dev/null @@ -1,366 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:0f6dea1f19194326599a9bca2989e912ed17e32f1ffb8d9305e16c13f8cacf2c" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "18: Radioactive decay" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.1, Page number 347" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "N0=1; #assume\n", - "\n", - "#Calculation\n", - "f=(N0/2)/N0; #fraction after t1/2\n", - "f1=(N0/4)/N0; #fraction after 2 half lives\n", - "f2=(N0/(2**5))/N0; #fraction after 5 half lives\n", - "f3=(N0/(2**10))/N0; #fraction after 10 half lives\n", - "\n", - "#Result\n", - "print \"fraction after 2 half lives is\",f1\n", - "print \"fraction after 5 half lives is\",f2\n", - "print \"fraction after 10 half lives is\",f3" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "fraction after 2 half lives is 0.25\n", - "fraction after 5 half lives is 0.03125\n", - "fraction after 10 half lives is 0.0009765625\n" - ] - } - ], - "prompt_number": 1 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.2, Page number 348" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "thalf=2.7*24*60*60; #half life(s)\n", - "m=1*10**-6; #mass(gm)\n", - "Na=6.02*10**23; #avagadro number(atoms/mol)\n", - "M=198; #molar mass(g/mol)\n", - "t=8*24*60*60;\n", - "\n", - "#Calculation\n", - "lamda=0.693/thalf; #decay constant(per sec)\n", - "N=m*Na/M; #number of nuclei(atoms)\n", - "A0=lamda*N; #activity(disintegrations per sec)\n", - "A=A0*math.exp(-lamda*t); #activity for 8 days(decays per sec)\n", - "\n", - "#Result\n", - "print \"decay constant is\",round(lamda*10**6,2),\"*10**-6 per sec\"\n", - "print \"activity is\",round(A0/10**9,2),\"*10**9 disintegrations per sec\"\n", - "print \"activity for 8 days is\",round(A/10**9,2),\"*10**9 decays per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "decay constant is 2.97 *10**-6 per sec\n", - "activity is 9.03 *10**9 disintegrations per sec\n", - "activity for 8 days is 1.16 *10**9 decays per sec\n" - ] - } - ], - "prompt_number": 10 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.3, Page number 348" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "thalf=5570*365*24*60*60; #half life(s)\n", - "dNbydt=3.7*10**10*2*10**-3; #number of decays per sec\n", - "m=14;\n", - "Na=6.02*10**23; #avagadro number(atoms/mol)\n", - "\n", - "#Calculation\n", - "lamda=0.693/thalf; #decay constant(per sec)\n", - "N=dNbydt/lamda; #number of atoms\n", - "mN=m*N/Na; #mass of 2mCi(g)\n", - "\n", - "#Result\n", - "print \"mass of 2mCi is\",round(mN*10**4,2),\"*10**-4 g\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "mass of 2mCi is 4.36 *10**-4 g\n" - ] - } - ], - "prompt_number": 23 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.5, Page number 353" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "thalf=1.25*10**9; #half life(yr)\n", - "r=10.2; #ratio of number of atoms\n", - "\n", - "#Calculation\n", - "a=1+r;\n", - "lamda=0.693/thalf; #decay constant(per yr)\n", - "t=math.log(a)/lamda; #time(yr)\n", - "\n", - "#Result\n", - "print \"the rock is\",round(t/10**9,2),\"*10**9 yrs old\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "the rock is 4.36 *10**9 yrs old\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.6, Page number 356" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mU=232.037131; #atomic mass of U(u)\n", - "mHe=4.002603; #atomic mass of He(u)\n", - "E=931.5; #energy(MeV)\n", - "KE=5.32; #kinetic energy of alpha particle(MeV)\n", - "\n", - "#Calculation\n", - "mTh=mU-mHe-(KE/E); #atomic mass of Th(u)\n", - "\n", - "#Result\n", - "print \"atomic mass of Th is\",round(mTh,5),\"u\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "atomic mass of Th is 228.02882 u\n" - ] - } - ], - "prompt_number": 14 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.7, Page number 359" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "E=931.5; #energy(MeV)\n", - "mX=11.011433; #mass of 11C(u)\n", - "mXdash=11.009305; #mass of 11B(u)\n", - "me=0.511;\n", - "\n", - "#Calculation\n", - "Q=(E*(mX-mXdash))-(2*me); #Q value for decay(MeV)\n", - "\n", - "#Result\n", - "print \"maximum energy is\",round(Q,2),\"MeV.minimum energy is zero\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "maximum energy is 0.96 MeV.minimum energy is zero\n" - ] - } - ], - "prompt_number": 16 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.8, Page number 359" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mK=39.963999; #mass of K(u)\n", - "mAr=39.962384; #mass of Ar(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "Q=(mK-mAr)*E; #kinetic energy of neutrino(MeV)\n", - "\n", - "#Result\n", - "print \"kinetic energy of neutrino is\",round(Q,3),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "kinetic energy of neutrino is 1.504 MeV\n" - ] - } - ], - "prompt_number": 18 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.9, Page number 360" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mN=12.018613; #mass of N(u)\n", - "mC=12; #mass of C(u)\n", - "me=0.000549; #mass of me(u)\n", - "E=931.5; #energy(MeV)\n", - "Egamma=4.43; #energy of emitted gamma ray(MeV)\n", - "\n", - "#Calculation\n", - "Q=(mN-mC-(2*me))*E; #Q value(MeV)\n", - "Emax=Q-Egamma; #maximum kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"maximum kinetic energy is\",round(Emax,2),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "maximum kinetic energy is 11.89 MeV\n" - ] - } - ], - "prompt_number": 20 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter18_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter18_2.ipynb deleted file mode 100755 index b99ff137..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter18_2.ipynb +++ /dev/null @@ -1,366 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:0f6dea1f19194326599a9bca2989e912ed17e32f1ffb8d9305e16c13f8cacf2c" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "18: Radioactive decay" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.1, Page number 347" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "N0=1; #assume\n", - "\n", - "#Calculation\n", - "f=(N0/2)/N0; #fraction after t1/2\n", - "f1=(N0/4)/N0; #fraction after 2 half lives\n", - "f2=(N0/(2**5))/N0; #fraction after 5 half lives\n", - "f3=(N0/(2**10))/N0; #fraction after 10 half lives\n", - "\n", - "#Result\n", - "print \"fraction after 2 half lives is\",f1\n", - "print \"fraction after 5 half lives is\",f2\n", - "print \"fraction after 10 half lives is\",f3" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "fraction after 2 half lives is 0.25\n", - "fraction after 5 half lives is 0.03125\n", - "fraction after 10 half lives is 0.0009765625\n" - ] - } - ], - "prompt_number": 1 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.2, Page number 348" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "thalf=2.7*24*60*60; #half life(s)\n", - "m=1*10**-6; #mass(gm)\n", - "Na=6.02*10**23; #avagadro number(atoms/mol)\n", - "M=198; #molar mass(g/mol)\n", - "t=8*24*60*60;\n", - "\n", - "#Calculation\n", - "lamda=0.693/thalf; #decay constant(per sec)\n", - "N=m*Na/M; #number of nuclei(atoms)\n", - "A0=lamda*N; #activity(disintegrations per sec)\n", - "A=A0*math.exp(-lamda*t); #activity for 8 days(decays per sec)\n", - "\n", - "#Result\n", - "print \"decay constant is\",round(lamda*10**6,2),\"*10**-6 per sec\"\n", - "print \"activity is\",round(A0/10**9,2),\"*10**9 disintegrations per sec\"\n", - "print \"activity for 8 days is\",round(A/10**9,2),\"*10**9 decays per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "decay constant is 2.97 *10**-6 per sec\n", - "activity is 9.03 *10**9 disintegrations per sec\n", - "activity for 8 days is 1.16 *10**9 decays per sec\n" - ] - } - ], - "prompt_number": 10 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.3, Page number 348" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "thalf=5570*365*24*60*60; #half life(s)\n", - "dNbydt=3.7*10**10*2*10**-3; #number of decays per sec\n", - "m=14;\n", - "Na=6.02*10**23; #avagadro number(atoms/mol)\n", - "\n", - "#Calculation\n", - "lamda=0.693/thalf; #decay constant(per sec)\n", - "N=dNbydt/lamda; #number of atoms\n", - "mN=m*N/Na; #mass of 2mCi(g)\n", - "\n", - "#Result\n", - "print \"mass of 2mCi is\",round(mN*10**4,2),\"*10**-4 g\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "mass of 2mCi is 4.36 *10**-4 g\n" - ] - } - ], - "prompt_number": 23 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.5, Page number 353" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "thalf=1.25*10**9; #half life(yr)\n", - "r=10.2; #ratio of number of atoms\n", - "\n", - "#Calculation\n", - "a=1+r;\n", - "lamda=0.693/thalf; #decay constant(per yr)\n", - "t=math.log(a)/lamda; #time(yr)\n", - "\n", - "#Result\n", - "print \"the rock is\",round(t/10**9,2),\"*10**9 yrs old\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "the rock is 4.36 *10**9 yrs old\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.6, Page number 356" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mU=232.037131; #atomic mass of U(u)\n", - "mHe=4.002603; #atomic mass of He(u)\n", - "E=931.5; #energy(MeV)\n", - "KE=5.32; #kinetic energy of alpha particle(MeV)\n", - "\n", - "#Calculation\n", - "mTh=mU-mHe-(KE/E); #atomic mass of Th(u)\n", - "\n", - "#Result\n", - "print \"atomic mass of Th is\",round(mTh,5),\"u\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "atomic mass of Th is 228.02882 u\n" - ] - } - ], - "prompt_number": 14 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.7, Page number 359" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "E=931.5; #energy(MeV)\n", - "mX=11.011433; #mass of 11C(u)\n", - "mXdash=11.009305; #mass of 11B(u)\n", - "me=0.511;\n", - "\n", - "#Calculation\n", - "Q=(E*(mX-mXdash))-(2*me); #Q value for decay(MeV)\n", - "\n", - "#Result\n", - "print \"maximum energy is\",round(Q,2),\"MeV.minimum energy is zero\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "maximum energy is 0.96 MeV.minimum energy is zero\n" - ] - } - ], - "prompt_number": 16 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.8, Page number 359" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mK=39.963999; #mass of K(u)\n", - "mAr=39.962384; #mass of Ar(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "Q=(mK-mAr)*E; #kinetic energy of neutrino(MeV)\n", - "\n", - "#Result\n", - "print \"kinetic energy of neutrino is\",round(Q,3),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "kinetic energy of neutrino is 1.504 MeV\n" - ] - } - ], - "prompt_number": 18 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 18.9, Page number 360" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mN=12.018613; #mass of N(u)\n", - "mC=12; #mass of C(u)\n", - "me=0.000549; #mass of me(u)\n", - "E=931.5; #energy(MeV)\n", - "Egamma=4.43; #energy of emitted gamma ray(MeV)\n", - "\n", - "#Calculation\n", - "Q=(mN-mC-(2*me))*E; #Q value(MeV)\n", - "Emax=Q-Egamma; #maximum kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"maximum kinetic energy is\",round(Emax,2),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "maximum kinetic energy is 11.89 MeV\n" - ] - } - ], - "prompt_number": 20 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter19.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter19.ipynb deleted file mode 100755 index c8745970..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter19.ipynb +++ /dev/null @@ -1,291 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:9326f276d5dc99ce97d41c9ca0d5924dbd68f522091536657f41d8cfe038dc31" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "19: Nuclear reactions" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.1, Page number 368" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m2H=2.014102; #atomic mass of 2H(u)\n", - "mn=1.008665; #mass of n(u)\n", - "m63Cu=62.929599; #mass of 63Cu(u)\n", - "m64Zn=63.929144; #mass of m64Zn(u)\n", - "E=931.5; #energy(MeV)\n", - "Kx=10; #energy of deutron(MeV)\n", - "Ky=15; #energy of neutron(MeV)\n", - "\n", - "#Calculation\n", - "Q=E*(m2H+m63Cu-mn-m64Zn); #Q-value(MeV)\n", - "KY=Q+Kx-Ky; #kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"Q-value is\",round(Q,3),\"MeV\"\n", - "print \"kinetic energy is\",round(KY,3),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Q-value is 5.488 MeV\n", - "kinetic energy is 0.488 MeV\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.2, Page number 368" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m19F=18.998404; #atomic mass of 19F(u)\n", - "mH=1.007825; #mass of H(u)\n", - "m19O=19.003577; #mass of 19O(u)\n", - "mn=1.008665; #mass of n(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "Q=E*(m19F+mn-mH-m19O); #Q-value(MeV)\n", - "Kxmin=-Q*(1+(mn/m19F)); #threshold energy(MeV)\n", - "\n", - "#Result\n", - "print \"Q-value is\",round(Q,4),\"MeV\"\n", - "print \"threshold energy is\",round(Kxmin,2),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Q-value is -4.0362 MeV\n", - "threshold energy is 4.25 MeV\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.3, Page number 373" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mn=1.008665; #mass of n(u)\n", - "mu=235.043924; #mass of 235U(u)\n", - "mBa=140.91440; #mass of 141Ba(u)\n", - "mKr=91.92630; #mass of Kr(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "mr=mn+mu; #mass of reactants(u)\n", - "mp=mBa+mKr+(3*mn); #mass of products(u)\n", - "md=mr-mp; #mass difference(u)\n", - "E=md*E; #energy released(MeV)\n", - "\n", - "#Result\n", - "print \"energy released is\",round(E,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy released is 173.2 MeV\n" - ] - } - ], - "prompt_number": 19 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.4, Page number 373" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "E=200*10**6; #energy released(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "P=300*10**6; #power(W)\n", - "t=1; #time(s)\n", - "\n", - "#Calculation\n", - "n=P*t/(E*e); #number of fissions per second\n", - "\n", - "#Result\n", - "print \"number of fissions per second is\",n" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number of fissions per second is 9.375e+18\n" - ] - } - ], - "prompt_number": 20 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.5, Page number 378" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m2H1=2*1.66*10**-27; #mass of proton(kg)\n", - "E=931.5; #energy(MeV)\n", - "m1=2.014102;\n", - "m2=3.01609;\n", - "mH=1.007825; #mass of H(u)\n", - "\n", - "#Calculation\n", - "E=E*((2*m1)-m2-mH); #energy released(MeV)\n", - "n=0.001/m2H1; #number of nuclei\n", - "Eg=n*E/2; #energy released per gm(MeV)\n", - "\n", - "#Result\n", - "print \"energy released per gm is\",round(Eg/10**23,2),\"*10**23 MeV\"\n", - "print \"answer given in the book is wrong\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy released per gm is 6.02 *10**23 MeV\n", - "answer given in the book is wrong\n" - ] - } - ], - "prompt_number": 31 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.6, Page number 379" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=8.99*10**9; #value of k(Nm**2/C**2)\n", - "rd=1.5*10**-15; #radius of deuterium nucleus(m)\n", - "rt=1.7*10**-15; #radius of tritium nucleus(m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "KE=0.225; #kinetic energy for 1 particle(MeV)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "\n", - "#Calculation\n", - "K_E=k*e**2/(e*(rd+rt)); #kinetic energy of 2 particles(MeV)\n", - "T=2*KE*e*10**6/(3*k); #temperature(K)\n", - "\n", - "#Result\n", - "print \"temperature is\",round(T/10**9),\"*10**9 K\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "temperature is 2.0 *10**9 K\n" - ] - } - ], - "prompt_number": 35 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter19_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter19_1.ipynb deleted file mode 100755 index c8745970..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter19_1.ipynb +++ /dev/null @@ -1,291 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:9326f276d5dc99ce97d41c9ca0d5924dbd68f522091536657f41d8cfe038dc31" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "19: Nuclear reactions" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.1, Page number 368" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m2H=2.014102; #atomic mass of 2H(u)\n", - "mn=1.008665; #mass of n(u)\n", - "m63Cu=62.929599; #mass of 63Cu(u)\n", - "m64Zn=63.929144; #mass of m64Zn(u)\n", - "E=931.5; #energy(MeV)\n", - "Kx=10; #energy of deutron(MeV)\n", - "Ky=15; #energy of neutron(MeV)\n", - "\n", - "#Calculation\n", - "Q=E*(m2H+m63Cu-mn-m64Zn); #Q-value(MeV)\n", - "KY=Q+Kx-Ky; #kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"Q-value is\",round(Q,3),\"MeV\"\n", - "print \"kinetic energy is\",round(KY,3),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Q-value is 5.488 MeV\n", - "kinetic energy is 0.488 MeV\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.2, Page number 368" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m19F=18.998404; #atomic mass of 19F(u)\n", - "mH=1.007825; #mass of H(u)\n", - "m19O=19.003577; #mass of 19O(u)\n", - "mn=1.008665; #mass of n(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "Q=E*(m19F+mn-mH-m19O); #Q-value(MeV)\n", - "Kxmin=-Q*(1+(mn/m19F)); #threshold energy(MeV)\n", - "\n", - "#Result\n", - "print \"Q-value is\",round(Q,4),\"MeV\"\n", - "print \"threshold energy is\",round(Kxmin,2),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Q-value is -4.0362 MeV\n", - "threshold energy is 4.25 MeV\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.3, Page number 373" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mn=1.008665; #mass of n(u)\n", - "mu=235.043924; #mass of 235U(u)\n", - "mBa=140.91440; #mass of 141Ba(u)\n", - "mKr=91.92630; #mass of Kr(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "mr=mn+mu; #mass of reactants(u)\n", - "mp=mBa+mKr+(3*mn); #mass of products(u)\n", - "md=mr-mp; #mass difference(u)\n", - "E=md*E; #energy released(MeV)\n", - "\n", - "#Result\n", - "print \"energy released is\",round(E,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy released is 173.2 MeV\n" - ] - } - ], - "prompt_number": 19 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.4, Page number 373" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "E=200*10**6; #energy released(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "P=300*10**6; #power(W)\n", - "t=1; #time(s)\n", - "\n", - "#Calculation\n", - "n=P*t/(E*e); #number of fissions per second\n", - "\n", - "#Result\n", - "print \"number of fissions per second is\",n" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number of fissions per second is 9.375e+18\n" - ] - } - ], - "prompt_number": 20 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.5, Page number 378" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m2H1=2*1.66*10**-27; #mass of proton(kg)\n", - "E=931.5; #energy(MeV)\n", - "m1=2.014102;\n", - "m2=3.01609;\n", - "mH=1.007825; #mass of H(u)\n", - "\n", - "#Calculation\n", - "E=E*((2*m1)-m2-mH); #energy released(MeV)\n", - "n=0.001/m2H1; #number of nuclei\n", - "Eg=n*E/2; #energy released per gm(MeV)\n", - "\n", - "#Result\n", - "print \"energy released per gm is\",round(Eg/10**23,2),\"*10**23 MeV\"\n", - "print \"answer given in the book is wrong\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy released per gm is 6.02 *10**23 MeV\n", - "answer given in the book is wrong\n" - ] - } - ], - "prompt_number": 31 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.6, Page number 379" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=8.99*10**9; #value of k(Nm**2/C**2)\n", - "rd=1.5*10**-15; #radius of deuterium nucleus(m)\n", - "rt=1.7*10**-15; #radius of tritium nucleus(m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "KE=0.225; #kinetic energy for 1 particle(MeV)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "\n", - "#Calculation\n", - "K_E=k*e**2/(e*(rd+rt)); #kinetic energy of 2 particles(MeV)\n", - "T=2*KE*e*10**6/(3*k); #temperature(K)\n", - "\n", - "#Result\n", - "print \"temperature is\",round(T/10**9),\"*10**9 K\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "temperature is 2.0 *10**9 K\n" - ] - } - ], - "prompt_number": 35 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter19_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter19_2.ipynb deleted file mode 100755 index c8745970..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter19_2.ipynb +++ /dev/null @@ -1,291 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:9326f276d5dc99ce97d41c9ca0d5924dbd68f522091536657f41d8cfe038dc31" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "19: Nuclear reactions" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.1, Page number 368" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m2H=2.014102; #atomic mass of 2H(u)\n", - "mn=1.008665; #mass of n(u)\n", - "m63Cu=62.929599; #mass of 63Cu(u)\n", - "m64Zn=63.929144; #mass of m64Zn(u)\n", - "E=931.5; #energy(MeV)\n", - "Kx=10; #energy of deutron(MeV)\n", - "Ky=15; #energy of neutron(MeV)\n", - "\n", - "#Calculation\n", - "Q=E*(m2H+m63Cu-mn-m64Zn); #Q-value(MeV)\n", - "KY=Q+Kx-Ky; #kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"Q-value is\",round(Q,3),\"MeV\"\n", - "print \"kinetic energy is\",round(KY,3),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Q-value is 5.488 MeV\n", - "kinetic energy is 0.488 MeV\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.2, Page number 368" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m19F=18.998404; #atomic mass of 19F(u)\n", - "mH=1.007825; #mass of H(u)\n", - "m19O=19.003577; #mass of 19O(u)\n", - "mn=1.008665; #mass of n(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "Q=E*(m19F+mn-mH-m19O); #Q-value(MeV)\n", - "Kxmin=-Q*(1+(mn/m19F)); #threshold energy(MeV)\n", - "\n", - "#Result\n", - "print \"Q-value is\",round(Q,4),\"MeV\"\n", - "print \"threshold energy is\",round(Kxmin,2),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Q-value is -4.0362 MeV\n", - "threshold energy is 4.25 MeV\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.3, Page number 373" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mn=1.008665; #mass of n(u)\n", - "mu=235.043924; #mass of 235U(u)\n", - "mBa=140.91440; #mass of 141Ba(u)\n", - "mKr=91.92630; #mass of Kr(u)\n", - "E=931.5; #energy(MeV)\n", - "\n", - "#Calculation\n", - "mr=mn+mu; #mass of reactants(u)\n", - "mp=mBa+mKr+(3*mn); #mass of products(u)\n", - "md=mr-mp; #mass difference(u)\n", - "E=md*E; #energy released(MeV)\n", - "\n", - "#Result\n", - "print \"energy released is\",round(E,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy released is 173.2 MeV\n" - ] - } - ], - "prompt_number": 19 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.4, Page number 373" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "E=200*10**6; #energy released(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "P=300*10**6; #power(W)\n", - "t=1; #time(s)\n", - "\n", - "#Calculation\n", - "n=P*t/(E*e); #number of fissions per second\n", - "\n", - "#Result\n", - "print \"number of fissions per second is\",n" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number of fissions per second is 9.375e+18\n" - ] - } - ], - "prompt_number": 20 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.5, Page number 378" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m2H1=2*1.66*10**-27; #mass of proton(kg)\n", - "E=931.5; #energy(MeV)\n", - "m1=2.014102;\n", - "m2=3.01609;\n", - "mH=1.007825; #mass of H(u)\n", - "\n", - "#Calculation\n", - "E=E*((2*m1)-m2-mH); #energy released(MeV)\n", - "n=0.001/m2H1; #number of nuclei\n", - "Eg=n*E/2; #energy released per gm(MeV)\n", - "\n", - "#Result\n", - "print \"energy released per gm is\",round(Eg/10**23,2),\"*10**23 MeV\"\n", - "print \"answer given in the book is wrong\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy released per gm is 6.02 *10**23 MeV\n", - "answer given in the book is wrong\n" - ] - } - ], - "prompt_number": 31 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 19.6, Page number 379" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=8.99*10**9; #value of k(Nm**2/C**2)\n", - "rd=1.5*10**-15; #radius of deuterium nucleus(m)\n", - "rt=1.7*10**-15; #radius of tritium nucleus(m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "KE=0.225; #kinetic energy for 1 particle(MeV)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "\n", - "#Calculation\n", - "K_E=k*e**2/(e*(rd+rt)); #kinetic energy of 2 particles(MeV)\n", - "T=2*KE*e*10**6/(3*k); #temperature(K)\n", - "\n", - "#Result\n", - "print \"temperature is\",round(T/10**9),\"*10**9 K\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "temperature is 2.0 *10**9 K\n" - ] - } - ], - "prompt_number": 35 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter1_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter1_1.ipynb deleted file mode 100755 index 483d55f3..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter1_1.ipynb +++ /dev/null @@ -1,311 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:467ef5c6562d2c93b60e422b9b9a8c5a34323da84f6c33e87f513c3c578db36d" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "1: The special theory of relativity" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.2, Page number 10" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=1; #assume\n", - "udash=0.9*c; #speed of 2nd rocket\n", - "v=0.6*c; #speed of 1st rocket\n", - "\n", - "#Calculation\n", - "u1=(udash+v)/(1+(udash*v/(c**2))); #speed of 2nd rocket in same direction\n", - "u2=(-udash+v)/(1-(udash*v/(c**2))); #speed of 2nd rocket in opposite direction\n", - "\n", - "#Result\n", - "print \"speed of 2nd rocket in same direction is\",round(u1,3),\"*c\"\n", - "print \"speed of 2nd rocket in opposite direction is\",round(u2,3),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of 2nd rocket in same direction is 0.974 *c\n", - "speed of 2nd rocket in opposite direction is -0.652 *c\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.3, Page number 12" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "#given L0-L/L0=0.01.so L=0.99*L0\n", - "LbyL0=0.99;\n", - "c=1; #assume\n", - "\n", - "#Calculation\n", - "v2=(c**2)*(1-(LbyL0)**2);\n", - "v=math.sqrt(v2); #speed\n", - "\n", - "#Result\n", - "print \"speed is\",round(v,3),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed is 0.141 *c\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.4, Page number 12" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "delta_tow=2.6*10**-8; #mean lifetime at rest(s)\n", - "d=20; #distance(m)\n", - "c=3*10**8; #speed of light(m/s)\n", - "\n", - "#Calculation\n", - "#delta_t=d/v\n", - "v2=(c**2)/(1+(delta_tow*c/d)**2);\n", - "v=math.sqrt(v2); #speed of unstable particle(m/s)\n", - "\n", - "#Result\n", - "print \"speed of unstable particle is\",round(v/10**8,1),\"*10**8 m/s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of unstable particle is 2.8 *10**8 m/s\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.5, Page number 13" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "delta_t=5*10**-6; #mean lifetime(s)\n", - "c=1; #assume\n", - "v=0.9*c; #speed of beam\n", - "\n", - "#Calculation\n", - "delta_tow=delta_t*math.sqrt(1-(v/c)**2); #proper lifetime of particles(s)\n", - "\n", - "#Result\n", - "print \"proper lifetime of particles is\",round(delta_tow*10**6,2),\"*10**-6 s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "proper lifetime of particles is 2.18 *10**-6 s\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.6, Page number 15" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=1; #assume\n", - "m0bym=100/120; #ratio of masses\n", - "\n", - "#Calculation\n", - "v=c*math.sqrt(1-(m0bym**2)); #speed of body\n", - "\n", - "#Result\n", - "print \"speed of body is\",round(v,3),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of body is 0.553 *c\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.7, Page number 17" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=3*10**8; #speed of light(m/s)\n", - "deltaE=4*10**26; #energy of sun(J/s)\n", - "\n", - "#Calculation\n", - "deltam=deltaE/c**2; #change in mass(kg)\n", - "\n", - "#Result\n", - "print \"change in mass is\",round(deltam/10**9,2),\"*10**9 kg\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "change in mass is 4.44 *10**9 kg\n" - ] - } - ], - "prompt_number": 13 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.8, Page number 17" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=1; #assume\n", - "T=10; #kinetic energy(MeV)\n", - "m0c2=0.512; #rest energy of electron(MeV)\n", - "\n", - "#Calculation\n", - "E=T+m0c2; #total energy(MeV)\n", - "p=math.sqrt((E**2)-(m0c2**2))/c; #momentum of electron(MeV/c)\n", - "v=c*math.sqrt(1-(m0c2/E)**2); #velocity of electron(c)\n", - "\n", - "#Result\n", - "print \"momentum of electron is\",round(p,1),\"MeV/c\"\n", - "print \"velocity of electron is\",round(v,4),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "momentum of electron is 10.5 MeV/c\n", - "velocity of electron is 0.9988 *c\n" - ] - } - ], - "prompt_number": 16 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter1_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter1_2.ipynb deleted file mode 100755 index 483d55f3..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter1_2.ipynb +++ /dev/null @@ -1,311 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:467ef5c6562d2c93b60e422b9b9a8c5a34323da84f6c33e87f513c3c578db36d" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "1: The special theory of relativity" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.2, Page number 10" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=1; #assume\n", - "udash=0.9*c; #speed of 2nd rocket\n", - "v=0.6*c; #speed of 1st rocket\n", - "\n", - "#Calculation\n", - "u1=(udash+v)/(1+(udash*v/(c**2))); #speed of 2nd rocket in same direction\n", - "u2=(-udash+v)/(1-(udash*v/(c**2))); #speed of 2nd rocket in opposite direction\n", - "\n", - "#Result\n", - "print \"speed of 2nd rocket in same direction is\",round(u1,3),\"*c\"\n", - "print \"speed of 2nd rocket in opposite direction is\",round(u2,3),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of 2nd rocket in same direction is 0.974 *c\n", - "speed of 2nd rocket in opposite direction is -0.652 *c\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.3, Page number 12" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "#given L0-L/L0=0.01.so L=0.99*L0\n", - "LbyL0=0.99;\n", - "c=1; #assume\n", - "\n", - "#Calculation\n", - "v2=(c**2)*(1-(LbyL0)**2);\n", - "v=math.sqrt(v2); #speed\n", - "\n", - "#Result\n", - "print \"speed is\",round(v,3),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed is 0.141 *c\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.4, Page number 12" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "delta_tow=2.6*10**-8; #mean lifetime at rest(s)\n", - "d=20; #distance(m)\n", - "c=3*10**8; #speed of light(m/s)\n", - "\n", - "#Calculation\n", - "#delta_t=d/v\n", - "v2=(c**2)/(1+(delta_tow*c/d)**2);\n", - "v=math.sqrt(v2); #speed of unstable particle(m/s)\n", - "\n", - "#Result\n", - "print \"speed of unstable particle is\",round(v/10**8,1),\"*10**8 m/s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of unstable particle is 2.8 *10**8 m/s\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.5, Page number 13" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "delta_t=5*10**-6; #mean lifetime(s)\n", - "c=1; #assume\n", - "v=0.9*c; #speed of beam\n", - "\n", - "#Calculation\n", - "delta_tow=delta_t*math.sqrt(1-(v/c)**2); #proper lifetime of particles(s)\n", - "\n", - "#Result\n", - "print \"proper lifetime of particles is\",round(delta_tow*10**6,2),\"*10**-6 s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "proper lifetime of particles is 2.18 *10**-6 s\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.6, Page number 15" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=1; #assume\n", - "m0bym=100/120; #ratio of masses\n", - "\n", - "#Calculation\n", - "v=c*math.sqrt(1-(m0bym**2)); #speed of body\n", - "\n", - "#Result\n", - "print \"speed of body is\",round(v,3),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "speed of body is 0.553 *c\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.7, Page number 17" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=3*10**8; #speed of light(m/s)\n", - "deltaE=4*10**26; #energy of sun(J/s)\n", - "\n", - "#Calculation\n", - "deltam=deltaE/c**2; #change in mass(kg)\n", - "\n", - "#Result\n", - "print \"change in mass is\",round(deltam/10**9,2),\"*10**9 kg\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "change in mass is 4.44 *10**9 kg\n" - ] - } - ], - "prompt_number": 13 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 1.8, Page number 17" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=1; #assume\n", - "T=10; #kinetic energy(MeV)\n", - "m0c2=0.512; #rest energy of electron(MeV)\n", - "\n", - "#Calculation\n", - "E=T+m0c2; #total energy(MeV)\n", - "p=math.sqrt((E**2)-(m0c2**2))/c; #momentum of electron(MeV/c)\n", - "v=c*math.sqrt(1-(m0c2/E)**2); #velocity of electron(c)\n", - "\n", - "#Result\n", - "print \"momentum of electron is\",round(p,1),\"MeV/c\"\n", - "print \"velocity of electron is\",round(v,4),\"*c\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "momentum of electron is 10.5 MeV/c\n", - "velocity of electron is 0.9988 *c\n" - ] - } - ], - "prompt_number": 16 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter2.ipynb deleted file mode 100755 index 59d9ea57..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter2.ipynb +++ /dev/null @@ -1,295 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:f048d58df41f2578c151ef59f03652004b6758b9e666d170255be2c66115bfe2" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "2: Particle nature of radiation" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.1, Page number 28" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new=100*10**6; #frequency(Hz)\n", - "P=100*10**3; #power(watt)\n", - "\n", - "#Calculation\n", - "E=h*new; #quantum of energy(J)\n", - "n=P/E; #number of quanta emitted(per sec)\n", - "\n", - "#Result\n", - "print \"number of quanta emitted is\",round(n/10**29,2),\"*10**29 per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number of quanta emitted is 15.09 *10**29 per sec\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.2, Page number 31" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=400*10**-9; #wavelength(m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "w0=2.28; #work function(eV)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "E=h*c/(lamda*e); #energy(eV)\n", - "KEmax=E-w0; #maximum kinetic energy(eV)\n", - "v2=2*KEmax*e/m; \n", - "v=math.sqrt(v2); #velocity(m/s)\n", - "\n", - "#Result\n", - "print \"maximum kinetic energy is\",round(KEmax,3),\"eV\"\n", - "print \"velocity of photoelectrons is\",round(v/10**5,2),\"*10**5 m/s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "maximum kinetic energy is 0.826 eV\n", - "velocity of photoelectrons is 5.39 *10**5 m/s\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.3, Page number 31" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=2000*10**-10; #wavelength(m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "w0=4.2; #work function(eV)\n", - "\n", - "#Calculation\n", - "lamda0=h*c/(w0*e); #cut off wavelength(m)\n", - "E=h*c/(lamda*e); #energy(eV)\n", - "sp=E-w0; #stopping potential(eV)\n", - "\n", - "#Result\n", - "print \"cut off wavelength is\",int(lamda0*10**10),\"angstrom\"\n", - "print \"stopping potential is\",round(sp,2),\"V\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "cut off wavelength is 2958 angstrom\n", - "stopping potential is 2.01 V\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.4, Page number 33" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=0.2*10**-9; #wavelength(m)\n", - "\n", - "#Calculation\n", - "p=h/lamda; #momentum(kg m/s)\n", - "m=p/c; #effective mass(kg)\n", - "\n", - "#Result\n", - "print \"momentum is\",round(p*10**24,1),\"*10**-24 kg m/s\"\n", - "print \"effective mass is\",round(m*10**32,1),\"*10**-32 kg\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "momentum is 3.3 *10**-24 kg m/s\n", - "effective mass is 1.1 *10**-32 kg\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.5, Page number 35" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=0.15; #wavelength(nm)\n", - "m0=9.1*10**-31; #mass of electron(kg)\n", - "theta1=0; #scattering angle1(degrees)\n", - "theta2=90; #scattering angle2(degrees)\n", - "theta3=180; #scattering angle3(degrees)\n", - "\n", - "#Calculation\n", - "theta1=theta1*math.pi/180; #scattering angle1(radian)\n", - "theta2=theta2*math.pi/180; #scattering angle2(radian)\n", - "theta3=theta3*math.pi/180; #scattering angle3(radian)\n", - "lamda_dash1=lamda+(h*(1-math.cos(theta1))/(m0*c)); #wavelength at 0(nm)\n", - "lamda_dash2=lamda+(10**9*h*(1-math.cos(theta2))/(m0*c)); #wavelength at 90(nm)\n", - "lamda_dash3=lamda+(10**9*h*(1-math.cos(theta3))/(m0*c)); #wavelength at 180(nm)\n", - "\n", - "#Result\n", - "print \"wavelength at 0 degrees is\",lamda_dash1,\"nm\"\n", - "print \"wavelength at 90 degrees is\",round(lamda_dash2,3),\"nm\"\n", - "print \"wavelength at 180 degrees is\",round(lamda_dash3,3),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength at 0 degrees is 0.15 nm\n", - "wavelength at 90 degrees is 0.152 nm\n", - "wavelength at 180 degrees is 0.155 nm\n" - ] - } - ], - "prompt_number": 18 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.6, Page number 36" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "E=2*0.511*10**6; #rest energy(eV)\n", - "\n", - "#Calculation\n", - "lamda=h*c/(E*e); #wavelength of photon(m)\n", - "\n", - "#Result\n", - "print \"wavelength of photon is\",round(lamda*10**12,2),\"*10**-12 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of photon is 1.22 *10**-12 m\n" - ] - } - ], - "prompt_number": 21 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter20.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter20.ipynb deleted file mode 100755 index 6f977e4e..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter20.ipynb +++ /dev/null @@ -1,119 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:eeb9c551735bd0ab45890fc906baf874437271bf852063fccc60d822b2aaeaef" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "20: Nuclear radiation detectors and particle accelerators" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 20.1, Page number 390" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=1.67*10**-27; #mass of proton(kg)\n", - "E=30*10**6; #energy(eV)\n", - "r=1.2*10**-15; #radius of nucleon(m)\n", - "\n", - "#Calculation\n", - "lamdaP=h/math.sqrt(2*m*E*e); #wavelength of proton(m)\n", - "lamdaAlpha=h/math.sqrt(2*4*m*E*e); #wavelength of alpha particle(m)\n", - "a=2*r; #size of nucleon(m)\n", - "\n", - "#Result\n", - "print \"wavelength of proton is\",round(lamdaP*10**15,1),\"*10**-15 m\"\n", - "print \"wavelength of alpha particle is\",round(lamdaAlpha*10**15,1),\"*10**-15 m\"\n", - "print \"size of nucleon is\",a,\"m\"\n", - "print \"alpha particle is better\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of proton is 5.2 *10**-15 m\n", - "wavelength of alpha particle is 2.6 *10**-15 m\n", - "size of nucleon is 2.4e-15 m\n", - "alpha particle is better\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 20.2, Page number 391" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "q=1.6*10**-19; #conversion factor from J to eV\n", - "B=2; #magnetic field(T)\n", - "m=1.67*10**-27; #mass of proton(kg)\n", - "R=0.25; #radius(m)\n", - "a=6.24*10**12; #conversion factor from J to MeV\n", - "\n", - "#Calculation\n", - "f=q*B/(2*math.pi*m); #frequency needed(MHz)\n", - "KE=q**2*B**2*R**2/(2*m); #kinetic energy(J)\n", - "KE=KE*a; #kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"frequency needed is\",round(f*10**-6,1),\"MHz\"\n", - "print \"kinetic energy is\",round(KE),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "frequency needed is 30.5 MHz\n", - "kinetic energy is 12.0 MeV\n" - ] - } - ], - "prompt_number": 8 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter20_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter20_1.ipynb deleted file mode 100755 index 6f977e4e..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter20_1.ipynb +++ /dev/null @@ -1,119 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:eeb9c551735bd0ab45890fc906baf874437271bf852063fccc60d822b2aaeaef" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "20: Nuclear radiation detectors and particle accelerators" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 20.1, Page number 390" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=1.67*10**-27; #mass of proton(kg)\n", - "E=30*10**6; #energy(eV)\n", - "r=1.2*10**-15; #radius of nucleon(m)\n", - "\n", - "#Calculation\n", - "lamdaP=h/math.sqrt(2*m*E*e); #wavelength of proton(m)\n", - "lamdaAlpha=h/math.sqrt(2*4*m*E*e); #wavelength of alpha particle(m)\n", - "a=2*r; #size of nucleon(m)\n", - "\n", - "#Result\n", - "print \"wavelength of proton is\",round(lamdaP*10**15,1),\"*10**-15 m\"\n", - "print \"wavelength of alpha particle is\",round(lamdaAlpha*10**15,1),\"*10**-15 m\"\n", - "print \"size of nucleon is\",a,\"m\"\n", - "print \"alpha particle is better\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of proton is 5.2 *10**-15 m\n", - "wavelength of alpha particle is 2.6 *10**-15 m\n", - "size of nucleon is 2.4e-15 m\n", - "alpha particle is better\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 20.2, Page number 391" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "q=1.6*10**-19; #conversion factor from J to eV\n", - "B=2; #magnetic field(T)\n", - "m=1.67*10**-27; #mass of proton(kg)\n", - "R=0.25; #radius(m)\n", - "a=6.24*10**12; #conversion factor from J to MeV\n", - "\n", - "#Calculation\n", - "f=q*B/(2*math.pi*m); #frequency needed(MHz)\n", - "KE=q**2*B**2*R**2/(2*m); #kinetic energy(J)\n", - "KE=KE*a; #kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"frequency needed is\",round(f*10**-6,1),\"MHz\"\n", - "print \"kinetic energy is\",round(KE),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "frequency needed is 30.5 MHz\n", - "kinetic energy is 12.0 MeV\n" - ] - } - ], - "prompt_number": 8 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter20_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter20_2.ipynb deleted file mode 100755 index 6f977e4e..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter20_2.ipynb +++ /dev/null @@ -1,119 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:eeb9c551735bd0ab45890fc906baf874437271bf852063fccc60d822b2aaeaef" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "20: Nuclear radiation detectors and particle accelerators" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 20.1, Page number 390" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=1.67*10**-27; #mass of proton(kg)\n", - "E=30*10**6; #energy(eV)\n", - "r=1.2*10**-15; #radius of nucleon(m)\n", - "\n", - "#Calculation\n", - "lamdaP=h/math.sqrt(2*m*E*e); #wavelength of proton(m)\n", - "lamdaAlpha=h/math.sqrt(2*4*m*E*e); #wavelength of alpha particle(m)\n", - "a=2*r; #size of nucleon(m)\n", - "\n", - "#Result\n", - "print \"wavelength of proton is\",round(lamdaP*10**15,1),\"*10**-15 m\"\n", - "print \"wavelength of alpha particle is\",round(lamdaAlpha*10**15,1),\"*10**-15 m\"\n", - "print \"size of nucleon is\",a,\"m\"\n", - "print \"alpha particle is better\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of proton is 5.2 *10**-15 m\n", - "wavelength of alpha particle is 2.6 *10**-15 m\n", - "size of nucleon is 2.4e-15 m\n", - "alpha particle is better\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 20.2, Page number 391" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "q=1.6*10**-19; #conversion factor from J to eV\n", - "B=2; #magnetic field(T)\n", - "m=1.67*10**-27; #mass of proton(kg)\n", - "R=0.25; #radius(m)\n", - "a=6.24*10**12; #conversion factor from J to MeV\n", - "\n", - "#Calculation\n", - "f=q*B/(2*math.pi*m); #frequency needed(MHz)\n", - "KE=q**2*B**2*R**2/(2*m); #kinetic energy(J)\n", - "KE=KE*a; #kinetic energy(MeV)\n", - "\n", - "#Result\n", - "print \"frequency needed is\",round(f*10**-6,1),\"MHz\"\n", - "print \"kinetic energy is\",round(KE),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "frequency needed is 30.5 MHz\n", - "kinetic energy is 12.0 MeV\n" - ] - } - ], - "prompt_number": 8 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter21.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter21.ipynb deleted file mode 100755 index 4e63e3b7..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter21.ipynb +++ /dev/null @@ -1,106 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:42eb4bd0fae1331d52fd855bad43219acea712dc31c5270f1f64fa698ba366ad" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "21: Elementary particles" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 21.1, Page number 399" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mpi=140; #mass of pi-meson\n", - "mp=938.3; #mass of proton\n", - "mk=498; #mass of k\n", - "m=1116; \n", - "\n", - "#Calculation\n", - "Q=mpi+mp-mk-m; #Q-value(MeV)\n", - "\n", - "#Result\n", - "print \"Q-value is\",round(Q),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Q-value is -536.0 MeV\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 21.2, Page number 399" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mpc2=938.3; #energy of proton(MeV)\n", - "Epic2=139.6; #energy of pi-meson(MeV)\n", - "mnc2=939.6; #energy of neutron(MeV)\n", - "KE=0.6; #kinetic energy of neutron(MeV)\n", - "\n", - "#Calculation\n", - "Epi=mpc2+Epic2-mnc2-KE; #energy conservation(MeV)\n", - "mpic2=math.sqrt((Epi**2)-((mnc2+KE)**2)+(mnc2**2)); #pi0 mass(MeV)\n", - "\n", - "#Result\n", - "print \"pi0 mass is\",round(mpic2,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "pi0 mass is 133.5 MeV\n" - ] - } - ], - "prompt_number": 5 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter21_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter21_1.ipynb deleted file mode 100755 index 4e63e3b7..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter21_1.ipynb +++ /dev/null @@ -1,106 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:42eb4bd0fae1331d52fd855bad43219acea712dc31c5270f1f64fa698ba366ad" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "21: Elementary particles" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 21.1, Page number 399" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mpi=140; #mass of pi-meson\n", - "mp=938.3; #mass of proton\n", - "mk=498; #mass of k\n", - "m=1116; \n", - "\n", - "#Calculation\n", - "Q=mpi+mp-mk-m; #Q-value(MeV)\n", - "\n", - "#Result\n", - "print \"Q-value is\",round(Q),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Q-value is -536.0 MeV\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 21.2, Page number 399" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mpc2=938.3; #energy of proton(MeV)\n", - "Epic2=139.6; #energy of pi-meson(MeV)\n", - "mnc2=939.6; #energy of neutron(MeV)\n", - "KE=0.6; #kinetic energy of neutron(MeV)\n", - "\n", - "#Calculation\n", - "Epi=mpc2+Epic2-mnc2-KE; #energy conservation(MeV)\n", - "mpic2=math.sqrt((Epi**2)-((mnc2+KE)**2)+(mnc2**2)); #pi0 mass(MeV)\n", - "\n", - "#Result\n", - "print \"pi0 mass is\",round(mpic2,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "pi0 mass is 133.5 MeV\n" - ] - } - ], - "prompt_number": 5 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter21_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter21_2.ipynb deleted file mode 100755 index 4e63e3b7..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter21_2.ipynb +++ /dev/null @@ -1,106 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:42eb4bd0fae1331d52fd855bad43219acea712dc31c5270f1f64fa698ba366ad" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "21: Elementary particles" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 21.1, Page number 399" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mpi=140; #mass of pi-meson\n", - "mp=938.3; #mass of proton\n", - "mk=498; #mass of k\n", - "m=1116; \n", - "\n", - "#Calculation\n", - "Q=mpi+mp-mk-m; #Q-value(MeV)\n", - "\n", - "#Result\n", - "print \"Q-value is\",round(Q),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Q-value is -536.0 MeV\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 21.2, Page number 399" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mpc2=938.3; #energy of proton(MeV)\n", - "Epic2=139.6; #energy of pi-meson(MeV)\n", - "mnc2=939.6; #energy of neutron(MeV)\n", - "KE=0.6; #kinetic energy of neutron(MeV)\n", - "\n", - "#Calculation\n", - "Epi=mpc2+Epic2-mnc2-KE; #energy conservation(MeV)\n", - "mpic2=math.sqrt((Epi**2)-((mnc2+KE)**2)+(mnc2**2)); #pi0 mass(MeV)\n", - "\n", - "#Result\n", - "print \"pi0 mass is\",round(mpic2,1),\"MeV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "pi0 mass is 133.5 MeV\n" - ] - } - ], - "prompt_number": 5 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter2_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter2_1.ipynb deleted file mode 100755 index 59d9ea57..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter2_1.ipynb +++ /dev/null @@ -1,295 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:f048d58df41f2578c151ef59f03652004b6758b9e666d170255be2c66115bfe2" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "2: Particle nature of radiation" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.1, Page number 28" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new=100*10**6; #frequency(Hz)\n", - "P=100*10**3; #power(watt)\n", - "\n", - "#Calculation\n", - "E=h*new; #quantum of energy(J)\n", - "n=P/E; #number of quanta emitted(per sec)\n", - "\n", - "#Result\n", - "print \"number of quanta emitted is\",round(n/10**29,2),\"*10**29 per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number of quanta emitted is 15.09 *10**29 per sec\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.2, Page number 31" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=400*10**-9; #wavelength(m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "w0=2.28; #work function(eV)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "E=h*c/(lamda*e); #energy(eV)\n", - "KEmax=E-w0; #maximum kinetic energy(eV)\n", - "v2=2*KEmax*e/m; \n", - "v=math.sqrt(v2); #velocity(m/s)\n", - "\n", - "#Result\n", - "print \"maximum kinetic energy is\",round(KEmax,3),\"eV\"\n", - "print \"velocity of photoelectrons is\",round(v/10**5,2),\"*10**5 m/s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "maximum kinetic energy is 0.826 eV\n", - "velocity of photoelectrons is 5.39 *10**5 m/s\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.3, Page number 31" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=2000*10**-10; #wavelength(m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "w0=4.2; #work function(eV)\n", - "\n", - "#Calculation\n", - "lamda0=h*c/(w0*e); #cut off wavelength(m)\n", - "E=h*c/(lamda*e); #energy(eV)\n", - "sp=E-w0; #stopping potential(eV)\n", - "\n", - "#Result\n", - "print \"cut off wavelength is\",int(lamda0*10**10),\"angstrom\"\n", - "print \"stopping potential is\",round(sp,2),\"V\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "cut off wavelength is 2958 angstrom\n", - "stopping potential is 2.01 V\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.4, Page number 33" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=0.2*10**-9; #wavelength(m)\n", - "\n", - "#Calculation\n", - "p=h/lamda; #momentum(kg m/s)\n", - "m=p/c; #effective mass(kg)\n", - "\n", - "#Result\n", - "print \"momentum is\",round(p*10**24,1),\"*10**-24 kg m/s\"\n", - "print \"effective mass is\",round(m*10**32,1),\"*10**-32 kg\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "momentum is 3.3 *10**-24 kg m/s\n", - "effective mass is 1.1 *10**-32 kg\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.5, Page number 35" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=0.15; #wavelength(nm)\n", - "m0=9.1*10**-31; #mass of electron(kg)\n", - "theta1=0; #scattering angle1(degrees)\n", - "theta2=90; #scattering angle2(degrees)\n", - "theta3=180; #scattering angle3(degrees)\n", - "\n", - "#Calculation\n", - "theta1=theta1*math.pi/180; #scattering angle1(radian)\n", - "theta2=theta2*math.pi/180; #scattering angle2(radian)\n", - "theta3=theta3*math.pi/180; #scattering angle3(radian)\n", - "lamda_dash1=lamda+(h*(1-math.cos(theta1))/(m0*c)); #wavelength at 0(nm)\n", - "lamda_dash2=lamda+(10**9*h*(1-math.cos(theta2))/(m0*c)); #wavelength at 90(nm)\n", - "lamda_dash3=lamda+(10**9*h*(1-math.cos(theta3))/(m0*c)); #wavelength at 180(nm)\n", - "\n", - "#Result\n", - "print \"wavelength at 0 degrees is\",lamda_dash1,\"nm\"\n", - "print \"wavelength at 90 degrees is\",round(lamda_dash2,3),\"nm\"\n", - "print \"wavelength at 180 degrees is\",round(lamda_dash3,3),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength at 0 degrees is 0.15 nm\n", - "wavelength at 90 degrees is 0.152 nm\n", - "wavelength at 180 degrees is 0.155 nm\n" - ] - } - ], - "prompt_number": 18 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.6, Page number 36" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "E=2*0.511*10**6; #rest energy(eV)\n", - "\n", - "#Calculation\n", - "lamda=h*c/(E*e); #wavelength of photon(m)\n", - "\n", - "#Result\n", - "print \"wavelength of photon is\",round(lamda*10**12,2),\"*10**-12 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of photon is 1.22 *10**-12 m\n" - ] - } - ], - "prompt_number": 21 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter2_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter2_2.ipynb deleted file mode 100755 index 59d9ea57..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter2_2.ipynb +++ /dev/null @@ -1,295 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:f048d58df41f2578c151ef59f03652004b6758b9e666d170255be2c66115bfe2" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "2: Particle nature of radiation" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.1, Page number 28" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new=100*10**6; #frequency(Hz)\n", - "P=100*10**3; #power(watt)\n", - "\n", - "#Calculation\n", - "E=h*new; #quantum of energy(J)\n", - "n=P/E; #number of quanta emitted(per sec)\n", - "\n", - "#Result\n", - "print \"number of quanta emitted is\",round(n/10**29,2),\"*10**29 per sec\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number of quanta emitted is 15.09 *10**29 per sec\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.2, Page number 31" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=400*10**-9; #wavelength(m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "w0=2.28; #work function(eV)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "\n", - "#Calculation\n", - "E=h*c/(lamda*e); #energy(eV)\n", - "KEmax=E-w0; #maximum kinetic energy(eV)\n", - "v2=2*KEmax*e/m; \n", - "v=math.sqrt(v2); #velocity(m/s)\n", - "\n", - "#Result\n", - "print \"maximum kinetic energy is\",round(KEmax,3),\"eV\"\n", - "print \"velocity of photoelectrons is\",round(v/10**5,2),\"*10**5 m/s\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "maximum kinetic energy is 0.826 eV\n", - "velocity of photoelectrons is 5.39 *10**5 m/s\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.3, Page number 31" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=2000*10**-10; #wavelength(m)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "w0=4.2; #work function(eV)\n", - "\n", - "#Calculation\n", - "lamda0=h*c/(w0*e); #cut off wavelength(m)\n", - "E=h*c/(lamda*e); #energy(eV)\n", - "sp=E-w0; #stopping potential(eV)\n", - "\n", - "#Result\n", - "print \"cut off wavelength is\",int(lamda0*10**10),\"angstrom\"\n", - "print \"stopping potential is\",round(sp,2),\"V\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "cut off wavelength is 2958 angstrom\n", - "stopping potential is 2.01 V\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.4, Page number 33" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=0.2*10**-9; #wavelength(m)\n", - "\n", - "#Calculation\n", - "p=h/lamda; #momentum(kg m/s)\n", - "m=p/c; #effective mass(kg)\n", - "\n", - "#Result\n", - "print \"momentum is\",round(p*10**24,1),\"*10**-24 kg m/s\"\n", - "print \"effective mass is\",round(m*10**32,1),\"*10**-32 kg\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "momentum is 3.3 *10**-24 kg m/s\n", - "effective mass is 1.1 *10**-32 kg\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.5, Page number 35" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=0.15; #wavelength(nm)\n", - "m0=9.1*10**-31; #mass of electron(kg)\n", - "theta1=0; #scattering angle1(degrees)\n", - "theta2=90; #scattering angle2(degrees)\n", - "theta3=180; #scattering angle3(degrees)\n", - "\n", - "#Calculation\n", - "theta1=theta1*math.pi/180; #scattering angle1(radian)\n", - "theta2=theta2*math.pi/180; #scattering angle2(radian)\n", - "theta3=theta3*math.pi/180; #scattering angle3(radian)\n", - "lamda_dash1=lamda+(h*(1-math.cos(theta1))/(m0*c)); #wavelength at 0(nm)\n", - "lamda_dash2=lamda+(10**9*h*(1-math.cos(theta2))/(m0*c)); #wavelength at 90(nm)\n", - "lamda_dash3=lamda+(10**9*h*(1-math.cos(theta3))/(m0*c)); #wavelength at 180(nm)\n", - "\n", - "#Result\n", - "print \"wavelength at 0 degrees is\",lamda_dash1,\"nm\"\n", - "print \"wavelength at 90 degrees is\",round(lamda_dash2,3),\"nm\"\n", - "print \"wavelength at 180 degrees is\",round(lamda_dash3,3),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength at 0 degrees is 0.15 nm\n", - "wavelength at 90 degrees is 0.152 nm\n", - "wavelength at 180 degrees is 0.155 nm\n" - ] - } - ], - "prompt_number": 18 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 2.6, Page number 36" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "E=2*0.511*10**6; #rest energy(eV)\n", - "\n", - "#Calculation\n", - "lamda=h*c/(E*e); #wavelength of photon(m)\n", - "\n", - "#Result\n", - "print \"wavelength of photon is\",round(lamda*10**12,2),\"*10**-12 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of photon is 1.22 *10**-12 m\n" - ] - } - ], - "prompt_number": 21 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter3.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter3.ipynb deleted file mode 100755 index 4d816cd2..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter3.ipynb +++ /dev/null @@ -1,197 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:b6d6dfa593701249cd6d305eb45cecde030c3502c19d325045b7e05cf46a035c" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "3: Atomic models" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.1, Page number 45" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "N=6.02*10**23; #avagadro number(atoms/mole)\n", - "rho=19.3; #density(g/cc)\n", - "A=197; #atomic weight(g)\n", - "k=8.984*10**9; #value of k(Nm**2/C**2)\n", - "Z=79;\n", - "Zdash=2;\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=2;\n", - "v0=8*10**6; \n", - "t=2*10**-6; #thickness(m)\n", - "\n", - "#Calculation\n", - "n=N*rho*10**6/A; #number of atoms(per m**3)\n", - "b=k*Z*Zdash*e/(m*v0); #impact parameter(m)\n", - "f=math.pi*b**2*n*t; #fraction of particles scattered\n", - "\n", - "#Result\n", - "print \"fraction of particles scattered is\",round(f*10**5,1),\"*10**-5\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "fraction of particles scattered is 7.5 *10**-5\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.3, Page number 48" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "E=10.5; #energy(eV)\n", - "\n", - "#Calculation\n", - "E=(13.6+E)*e; #energy of photon(J)\n", - "lamda=h*c/E; #wavelength(m)\n", - "\n", - "#Result\n", - "print \"wavelength of photon is\",round(lamda*10**9,2),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of photon is 51.55 nm\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.4, Page number 49" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=8.98*10**9; #value of k(Nm**2/C**2)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "n=1; #assume\n", - "a0=0.53*10**-10; #radius of orbit(m)\n", - "\n", - "#Calculation\n", - "PE=-k*(e**2)/(a0*e*n**2); #potential energy(eV)\n", - "E=-13.6/n**2; #energy(eV)\n", - "KE=E-PE; #kinetic energy(eV)\n", - "\n", - "#Result\n", - "print \"kinetic energy is\",round(KE,1),\"/n**2 eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "kinetic energy is 13.5 /n**2 eV\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.6, Page number 51" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "Mbyme=1836; \n", - "lamda=6562.8; #wavelength for hydrogen(angstrom)\n", - "\n", - "#Calculation\n", - "mew_dashbymew=2*(1+Mbyme)/(1+(2*Mbyme));\n", - "lamda_dash=lamda/mew_dashbymew; #wavelength for deuterium(angstrom)\n", - "\n", - "#Result\n", - "print \"wavelength for deuterium is\",int(lamda_dash),\"angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength for deuterium is 6561 angstrom\n" - ] - } - ], - "prompt_number": 14 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter3_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter3_1.ipynb deleted file mode 100755 index 4d816cd2..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter3_1.ipynb +++ /dev/null @@ -1,197 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:b6d6dfa593701249cd6d305eb45cecde030c3502c19d325045b7e05cf46a035c" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "3: Atomic models" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.1, Page number 45" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "N=6.02*10**23; #avagadro number(atoms/mole)\n", - "rho=19.3; #density(g/cc)\n", - "A=197; #atomic weight(g)\n", - "k=8.984*10**9; #value of k(Nm**2/C**2)\n", - "Z=79;\n", - "Zdash=2;\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=2;\n", - "v0=8*10**6; \n", - "t=2*10**-6; #thickness(m)\n", - "\n", - "#Calculation\n", - "n=N*rho*10**6/A; #number of atoms(per m**3)\n", - "b=k*Z*Zdash*e/(m*v0); #impact parameter(m)\n", - "f=math.pi*b**2*n*t; #fraction of particles scattered\n", - "\n", - "#Result\n", - "print \"fraction of particles scattered is\",round(f*10**5,1),\"*10**-5\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "fraction of particles scattered is 7.5 *10**-5\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.3, Page number 48" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "E=10.5; #energy(eV)\n", - "\n", - "#Calculation\n", - "E=(13.6+E)*e; #energy of photon(J)\n", - "lamda=h*c/E; #wavelength(m)\n", - "\n", - "#Result\n", - "print \"wavelength of photon is\",round(lamda*10**9,2),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of photon is 51.55 nm\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.4, Page number 49" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=8.98*10**9; #value of k(Nm**2/C**2)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "n=1; #assume\n", - "a0=0.53*10**-10; #radius of orbit(m)\n", - "\n", - "#Calculation\n", - "PE=-k*(e**2)/(a0*e*n**2); #potential energy(eV)\n", - "E=-13.6/n**2; #energy(eV)\n", - "KE=E-PE; #kinetic energy(eV)\n", - "\n", - "#Result\n", - "print \"kinetic energy is\",round(KE,1),\"/n**2 eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "kinetic energy is 13.5 /n**2 eV\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.6, Page number 51" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "Mbyme=1836; \n", - "lamda=6562.8; #wavelength for hydrogen(angstrom)\n", - "\n", - "#Calculation\n", - "mew_dashbymew=2*(1+Mbyme)/(1+(2*Mbyme));\n", - "lamda_dash=lamda/mew_dashbymew; #wavelength for deuterium(angstrom)\n", - "\n", - "#Result\n", - "print \"wavelength for deuterium is\",int(lamda_dash),\"angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength for deuterium is 6561 angstrom\n" - ] - } - ], - "prompt_number": 14 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter3_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter3_2.ipynb deleted file mode 100755 index 4d816cd2..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter3_2.ipynb +++ /dev/null @@ -1,197 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:b6d6dfa593701249cd6d305eb45cecde030c3502c19d325045b7e05cf46a035c" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "3: Atomic models" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.1, Page number 45" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "N=6.02*10**23; #avagadro number(atoms/mole)\n", - "rho=19.3; #density(g/cc)\n", - "A=197; #atomic weight(g)\n", - "k=8.984*10**9; #value of k(Nm**2/C**2)\n", - "Z=79;\n", - "Zdash=2;\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=2;\n", - "v0=8*10**6; \n", - "t=2*10**-6; #thickness(m)\n", - "\n", - "#Calculation\n", - "n=N*rho*10**6/A; #number of atoms(per m**3)\n", - "b=k*Z*Zdash*e/(m*v0); #impact parameter(m)\n", - "f=math.pi*b**2*n*t; #fraction of particles scattered\n", - "\n", - "#Result\n", - "print \"fraction of particles scattered is\",round(f*10**5,1),\"*10**-5\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "fraction of particles scattered is 7.5 *10**-5\n" - ] - } - ], - "prompt_number": 7 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.3, Page number 48" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "E=10.5; #energy(eV)\n", - "\n", - "#Calculation\n", - "E=(13.6+E)*e; #energy of photon(J)\n", - "lamda=h*c/E; #wavelength(m)\n", - "\n", - "#Result\n", - "print \"wavelength of photon is\",round(lamda*10**9,2),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength of photon is 51.55 nm\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.4, Page number 49" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "k=8.98*10**9; #value of k(Nm**2/C**2)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "n=1; #assume\n", - "a0=0.53*10**-10; #radius of orbit(m)\n", - "\n", - "#Calculation\n", - "PE=-k*(e**2)/(a0*e*n**2); #potential energy(eV)\n", - "E=-13.6/n**2; #energy(eV)\n", - "KE=E-PE; #kinetic energy(eV)\n", - "\n", - "#Result\n", - "print \"kinetic energy is\",round(KE,1),\"/n**2 eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "kinetic energy is 13.5 /n**2 eV\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 3.6, Page number 51" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "Mbyme=1836; \n", - "lamda=6562.8; #wavelength for hydrogen(angstrom)\n", - "\n", - "#Calculation\n", - "mew_dashbymew=2*(1+Mbyme)/(1+(2*Mbyme));\n", - "lamda_dash=lamda/mew_dashbymew; #wavelength for deuterium(angstrom)\n", - "\n", - "#Result\n", - "print \"wavelength for deuterium is\",int(lamda_dash),\"angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "wavelength for deuterium is 6561 angstrom\n" - ] - } - ], - "prompt_number": 14 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter4.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter4.ipynb deleted file mode 100755 index 350acf21..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter4.ipynb +++ /dev/null @@ -1,193 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:1d6457e2a94e0fa2b026a0acb8ba4fab526573258ee2c274c4328b7f611fb97a" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "4: Wave mechanical concepts" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.1, Page number 59" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "V=1; #assume\n", - "\n", - "#Calculation\n", - "lamda=h/math.sqrt(2*m*e*V); #debroglie wavelength(m)\n", - "\n", - "#Result\n", - "print \"debroglie wavelength is math.sqrt(\",int((lamda*10**10)**2),\"/V) angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "debroglie wavelength is math.sqrt( 150 /V) angstrom\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.2, Page number 59" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "KE=100*10**6; #kinetic energy(eV)\n", - "\n", - "#Calculation\n", - "p=math.sqrt(2*m*e); #momentum(kg m/s)\n", - "lamda1=h/p; #debroglie wavelength for 1 eV(m)\n", - "lamda2=h*c/(KE*e); #debroglie wavelength for 100 MeV(m)\n", - "\n", - "#Result\n", - "print \"debroglie wavelength for 1 eV is\",round(lamda1*10**9,1),\"nm\"\n", - "print \"debroglie wavelength for 100 MeV is\",round(lamda2*10**15,2),\"*10**-15 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "debroglie wavelength for 1 eV is 1.2 nm\n", - "debroglie wavelength for 100 MeV is 12.42 *10**-15 m\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.3, Page number 64" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "v=4*10**6; #speed of electron(m/s)\n", - "sp=1/100; #speed precision\n", - "hbar=1.05*10**-34; \n", - "\n", - "#Calculation\n", - "p=m*v; #momentum(kg m/s)\n", - "deltap=p*sp; #uncertainity in momentum(kg m/s)\n", - "deltax=hbar/(2*deltap); #precision in position(m)\n", - "\n", - "#Result\n", - "print \"precision in position is\",round(deltax*10**9,2),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "precision in position is 1.44 nm\n" - ] - } - ], - "prompt_number": 14 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.4, Page number 64" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=4000*10**-10; #wavelength(m)\n", - "deltat=10**-8; #average lifetime(s)\n", - "\n", - "#Calculation\n", - "delta_lamda=lamda**2/(4*math.pi*c*deltat); #width of line(m)\n", - "\n", - "#Result\n", - "print \"width of line is\",round(delta_lamda*10**15,2),\"*10**-15 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "width of line is 4.24 *10**-15 m\n" - ] - } - ], - "prompt_number": 16 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter4_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter4_1.ipynb deleted file mode 100755 index 350acf21..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter4_1.ipynb +++ /dev/null @@ -1,193 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:1d6457e2a94e0fa2b026a0acb8ba4fab526573258ee2c274c4328b7f611fb97a" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "4: Wave mechanical concepts" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.1, Page number 59" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "V=1; #assume\n", - "\n", - "#Calculation\n", - "lamda=h/math.sqrt(2*m*e*V); #debroglie wavelength(m)\n", - "\n", - "#Result\n", - "print \"debroglie wavelength is math.sqrt(\",int((lamda*10**10)**2),\"/V) angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "debroglie wavelength is math.sqrt( 150 /V) angstrom\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.2, Page number 59" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "KE=100*10**6; #kinetic energy(eV)\n", - "\n", - "#Calculation\n", - "p=math.sqrt(2*m*e); #momentum(kg m/s)\n", - "lamda1=h/p; #debroglie wavelength for 1 eV(m)\n", - "lamda2=h*c/(KE*e); #debroglie wavelength for 100 MeV(m)\n", - "\n", - "#Result\n", - "print \"debroglie wavelength for 1 eV is\",round(lamda1*10**9,1),\"nm\"\n", - "print \"debroglie wavelength for 100 MeV is\",round(lamda2*10**15,2),\"*10**-15 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "debroglie wavelength for 1 eV is 1.2 nm\n", - "debroglie wavelength for 100 MeV is 12.42 *10**-15 m\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.3, Page number 64" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "v=4*10**6; #speed of electron(m/s)\n", - "sp=1/100; #speed precision\n", - "hbar=1.05*10**-34; \n", - "\n", - "#Calculation\n", - "p=m*v; #momentum(kg m/s)\n", - "deltap=p*sp; #uncertainity in momentum(kg m/s)\n", - "deltax=hbar/(2*deltap); #precision in position(m)\n", - "\n", - "#Result\n", - "print \"precision in position is\",round(deltax*10**9,2),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "precision in position is 1.44 nm\n" - ] - } - ], - "prompt_number": 14 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.4, Page number 64" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=4000*10**-10; #wavelength(m)\n", - "deltat=10**-8; #average lifetime(s)\n", - "\n", - "#Calculation\n", - "delta_lamda=lamda**2/(4*math.pi*c*deltat); #width of line(m)\n", - "\n", - "#Result\n", - "print \"width of line is\",round(delta_lamda*10**15,2),\"*10**-15 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "width of line is 4.24 *10**-15 m\n" - ] - } - ], - "prompt_number": 16 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter4_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter4_2.ipynb deleted file mode 100755 index 350acf21..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter4_2.ipynb +++ /dev/null @@ -1,193 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:1d6457e2a94e0fa2b026a0acb8ba4fab526573258ee2c274c4328b7f611fb97a" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "4: Wave mechanical concepts" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.1, Page number 59" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "V=1; #assume\n", - "\n", - "#Calculation\n", - "lamda=h/math.sqrt(2*m*e*V); #debroglie wavelength(m)\n", - "\n", - "#Result\n", - "print \"debroglie wavelength is math.sqrt(\",int((lamda*10**10)**2),\"/V) angstrom\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "debroglie wavelength is math.sqrt( 150 /V) angstrom\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.2, Page number 59" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "KE=100*10**6; #kinetic energy(eV)\n", - "\n", - "#Calculation\n", - "p=math.sqrt(2*m*e); #momentum(kg m/s)\n", - "lamda1=h/p; #debroglie wavelength for 1 eV(m)\n", - "lamda2=h*c/(KE*e); #debroglie wavelength for 100 MeV(m)\n", - "\n", - "#Result\n", - "print \"debroglie wavelength for 1 eV is\",round(lamda1*10**9,1),\"nm\"\n", - "print \"debroglie wavelength for 100 MeV is\",round(lamda2*10**15,2),\"*10**-15 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "debroglie wavelength for 1 eV is 1.2 nm\n", - "debroglie wavelength for 100 MeV is 12.42 *10**-15 m\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.3, Page number 64" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "v=4*10**6; #speed of electron(m/s)\n", - "sp=1/100; #speed precision\n", - "hbar=1.05*10**-34; \n", - "\n", - "#Calculation\n", - "p=m*v; #momentum(kg m/s)\n", - "deltap=p*sp; #uncertainity in momentum(kg m/s)\n", - "deltax=hbar/(2*deltap); #precision in position(m)\n", - "\n", - "#Result\n", - "print \"precision in position is\",round(deltax*10**9,2),\"nm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "precision in position is 1.44 nm\n" - ] - } - ], - "prompt_number": 14 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 4.4, Page number 64" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda=4000*10**-10; #wavelength(m)\n", - "deltat=10**-8; #average lifetime(s)\n", - "\n", - "#Calculation\n", - "delta_lamda=lamda**2/(4*math.pi*c*deltat); #width of line(m)\n", - "\n", - "#Result\n", - "print \"width of line is\",round(delta_lamda*10**15,2),\"*10**-15 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "width of line is 4.24 *10**-15 m\n" - ] - } - ], - "prompt_number": 16 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter6.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter6.ipynb deleted file mode 100755 index fa8615c7..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter6.ipynb +++ /dev/null @@ -1,208 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:8884b20a8f08880d4a94501a9f3a466664f30ca1f04c541fe7d3a232f87a24bc" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "6: Quantum mechanics of simple systems" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.1, Page number 90" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from scipy.integrate import quad\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=2*10**-10; #length of square well(m)\n", - "\n", - "#Calculation\n", - "def intg(x):\n", - " return (2/a)*(math.sin(math.pi*x/a))**2\n", - "\n", - "S=quad(intg,0,0.25*10**-10)[0] #probability of finding the electron\n", - "\n", - "#Result\n", - "print \"probability of finding the electron is\",round(S,4)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "probability of finding the electron is 0.0125\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.2, Page number 96" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new0=6.43*10**13; #frequency(Hz)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "mew=1.1385*10**-26; #reduced mass(kg)\n", - "\n", - "#Calculation\n", - "E0=h*new0/2; #zero point energy(J)\n", - "E0=E0/e; #zero point energy(eV)\n", - "k=4*math.pi**2*new0**2*mew; #force constane(N/m)\n", - "\n", - "#Result\n", - "print \"zero point energy is\",round(E0,3),\"eV\"\n", - "print \"force constane is\",round(k),\"N/m\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "zero point energy is 0.133 eV\n", - "force constane is 1858.0 N/m\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.6, Page number 104" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m1=19.9217*10**-27; #mass of carbon atom(kg)\n", - "m2=26.5614*10**-27; #mass of oxygen atom(kg)\n", - "r=1.131*10**-10; #separation(m)\n", - "hbar=1.054*10**-34;\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "mew=(m1*m2)/(m1+m2); #reduced mass(kg)\n", - "I=mew*r**2; \n", - "deltaE=hbar**2/I; #energy difference(J)\n", - "deltaE=deltaE/e; #energy difference(eV)\n", - "\n", - "#Result\n", - "print \"energy difference is\",round(deltaE*10**4,2),\"*10**-4 eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy difference is 4.77 *10**-4 eV\n" - ] - } - ], - "prompt_number": 21 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.7, Page number 105" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m1=1;\n", - "m2=0;\n", - "m3=-1; #m-components\n", - "l=1;\n", - "\n", - "#Calculation\n", - "L=math.sqrt(l*(l+1)); #length of vector\n", - "theta1=math.acos(m1/L); #orientation for m=1(radian)\n", - "theta1=theta1*180/math.pi; #orientation for m=1(degrees)\n", - "theta2=math.acos(m2/L); #orientation for m=0(radian)\n", - "theta2=theta2*180/math.pi; #orientation for m=0(degrees)\n", - "theta3=math.acos(m3/L); #orientation for m=-1(radian)\n", - "theta3=theta3*180/math.pi; #orientation for m=-1(degrees)\n", - "\n", - "#Result\n", - "print \"orientation for m=1 is\",theta1,\"degrees\"\n", - "print \"orientation for m=0 is\",theta2,\"degrees\"\n", - "print \"orientation for m=-1 is\",theta3,\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "orientation for m=1 is 45.0 degrees\n", - "orientation for m=0 is 90.0 degrees\n", - "orientation for m=-1 is 135.0 degrees\n" - ] - } - ], - "prompt_number": 22 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter6_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter6_1.ipynb deleted file mode 100755 index fa8615c7..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter6_1.ipynb +++ /dev/null @@ -1,208 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:8884b20a8f08880d4a94501a9f3a466664f30ca1f04c541fe7d3a232f87a24bc" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "6: Quantum mechanics of simple systems" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.1, Page number 90" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from scipy.integrate import quad\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=2*10**-10; #length of square well(m)\n", - "\n", - "#Calculation\n", - "def intg(x):\n", - " return (2/a)*(math.sin(math.pi*x/a))**2\n", - "\n", - "S=quad(intg,0,0.25*10**-10)[0] #probability of finding the electron\n", - "\n", - "#Result\n", - "print \"probability of finding the electron is\",round(S,4)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "probability of finding the electron is 0.0125\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.2, Page number 96" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new0=6.43*10**13; #frequency(Hz)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "mew=1.1385*10**-26; #reduced mass(kg)\n", - "\n", - "#Calculation\n", - "E0=h*new0/2; #zero point energy(J)\n", - "E0=E0/e; #zero point energy(eV)\n", - "k=4*math.pi**2*new0**2*mew; #force constane(N/m)\n", - "\n", - "#Result\n", - "print \"zero point energy is\",round(E0,3),\"eV\"\n", - "print \"force constane is\",round(k),\"N/m\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "zero point energy is 0.133 eV\n", - "force constane is 1858.0 N/m\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.6, Page number 104" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m1=19.9217*10**-27; #mass of carbon atom(kg)\n", - "m2=26.5614*10**-27; #mass of oxygen atom(kg)\n", - "r=1.131*10**-10; #separation(m)\n", - "hbar=1.054*10**-34;\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "mew=(m1*m2)/(m1+m2); #reduced mass(kg)\n", - "I=mew*r**2; \n", - "deltaE=hbar**2/I; #energy difference(J)\n", - "deltaE=deltaE/e; #energy difference(eV)\n", - "\n", - "#Result\n", - "print \"energy difference is\",round(deltaE*10**4,2),\"*10**-4 eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy difference is 4.77 *10**-4 eV\n" - ] - } - ], - "prompt_number": 21 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.7, Page number 105" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m1=1;\n", - "m2=0;\n", - "m3=-1; #m-components\n", - "l=1;\n", - "\n", - "#Calculation\n", - "L=math.sqrt(l*(l+1)); #length of vector\n", - "theta1=math.acos(m1/L); #orientation for m=1(radian)\n", - "theta1=theta1*180/math.pi; #orientation for m=1(degrees)\n", - "theta2=math.acos(m2/L); #orientation for m=0(radian)\n", - "theta2=theta2*180/math.pi; #orientation for m=0(degrees)\n", - "theta3=math.acos(m3/L); #orientation for m=-1(radian)\n", - "theta3=theta3*180/math.pi; #orientation for m=-1(degrees)\n", - "\n", - "#Result\n", - "print \"orientation for m=1 is\",theta1,\"degrees\"\n", - "print \"orientation for m=0 is\",theta2,\"degrees\"\n", - "print \"orientation for m=-1 is\",theta3,\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "orientation for m=1 is 45.0 degrees\n", - "orientation for m=0 is 90.0 degrees\n", - "orientation for m=-1 is 135.0 degrees\n" - ] - } - ], - "prompt_number": 22 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter6_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter6_2.ipynb deleted file mode 100755 index fa8615c7..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter6_2.ipynb +++ /dev/null @@ -1,208 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:8884b20a8f08880d4a94501a9f3a466664f30ca1f04c541fe7d3a232f87a24bc" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "6: Quantum mechanics of simple systems" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.1, Page number 90" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from scipy.integrate import quad\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "a=2*10**-10; #length of square well(m)\n", - "\n", - "#Calculation\n", - "def intg(x):\n", - " return (2/a)*(math.sin(math.pi*x/a))**2\n", - "\n", - "S=quad(intg,0,0.25*10**-10)[0] #probability of finding the electron\n", - "\n", - "#Result\n", - "print \"probability of finding the electron is\",round(S,4)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "probability of finding the electron is 0.0125\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.2, Page number 96" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new0=6.43*10**13; #frequency(Hz)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "mew=1.1385*10**-26; #reduced mass(kg)\n", - "\n", - "#Calculation\n", - "E0=h*new0/2; #zero point energy(J)\n", - "E0=E0/e; #zero point energy(eV)\n", - "k=4*math.pi**2*new0**2*mew; #force constane(N/m)\n", - "\n", - "#Result\n", - "print \"zero point energy is\",round(E0,3),\"eV\"\n", - "print \"force constane is\",round(k),\"N/m\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "zero point energy is 0.133 eV\n", - "force constane is 1858.0 N/m\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 9 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.6, Page number 104" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m1=19.9217*10**-27; #mass of carbon atom(kg)\n", - "m2=26.5614*10**-27; #mass of oxygen atom(kg)\n", - "r=1.131*10**-10; #separation(m)\n", - "hbar=1.054*10**-34;\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "mew=(m1*m2)/(m1+m2); #reduced mass(kg)\n", - "I=mew*r**2; \n", - "deltaE=hbar**2/I; #energy difference(J)\n", - "deltaE=deltaE/e; #energy difference(eV)\n", - "\n", - "#Result\n", - "print \"energy difference is\",round(deltaE*10**4,2),\"*10**-4 eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy difference is 4.77 *10**-4 eV\n" - ] - } - ], - "prompt_number": 21 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 6.7, Page number 105" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m1=1;\n", - "m2=0;\n", - "m3=-1; #m-components\n", - "l=1;\n", - "\n", - "#Calculation\n", - "L=math.sqrt(l*(l+1)); #length of vector\n", - "theta1=math.acos(m1/L); #orientation for m=1(radian)\n", - "theta1=theta1*180/math.pi; #orientation for m=1(degrees)\n", - "theta2=math.acos(m2/L); #orientation for m=0(radian)\n", - "theta2=theta2*180/math.pi; #orientation for m=0(degrees)\n", - "theta3=math.acos(m3/L); #orientation for m=-1(radian)\n", - "theta3=theta3*180/math.pi; #orientation for m=-1(degrees)\n", - "\n", - "#Result\n", - "print \"orientation for m=1 is\",theta1,\"degrees\"\n", - "print \"orientation for m=0 is\",theta2,\"degrees\"\n", - "print \"orientation for m=-1 is\",theta3,\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "orientation for m=1 is 45.0 degrees\n", - "orientation for m=0 is 90.0 degrees\n", - "orientation for m=-1 is 135.0 degrees\n" - ] - } - ], - "prompt_number": 22 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter7.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter7.ipynb deleted file mode 100755 index 45ed5766..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter7.ipynb +++ /dev/null @@ -1,258 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:1e02050388cdd15ca19e058c38c307c0fd0b145ef71769674c045940ea70b08b" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "7: Atomic physics" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.1, Page number 113" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mewB=9.27*10**-24;\n", - "B=3; #magnetic field(T)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "E=2*mewB*B/e; #energy difference(eV)\n", - "\n", - "#Result\n", - "print \"energy difference is\",round(E*10**4,2),\"*10**-4 eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy difference is 3.48 *10**-4 eV\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.3, Page number 118" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "l=2;\n", - "s=1/2;\n", - "j1=2+(1/2);\n", - "j2=2-(1/2);\n", - "\n", - "#Calculation\n", - "L=math.sqrt(l*(l+1)); #value of L(hbar)\n", - "S=math.sqrt(s*(s+1)); #value of S(hbar)\n", - "J1=math.sqrt(j1*(j1+1)); #value of J for D5/2 state(hbar)\n", - "J2=math.sqrt(j2*(j2+1)); #value of J for D3/2 state(hbar)\n", - "costheta1=((j1*(j1+1))-(l*(l+1))-(s*(s+1)))/(2*L*S);\n", - "theta1=math.acos(costheta1); #angle between L and S for D5/2(radian)\n", - "theta1=theta1*180/math.pi; #angle between L and S for D5/2(degrees)\n", - "costheta2=((j2*(j2+1))-(l*(l+1))-(s*(s+1)))/(2*L*S);\n", - "theta2=math.acos(costheta2); #angle between L and S for D3/2(radian)\n", - "theta2=theta2*180/math.pi; #angle between L and S for D3/2(degrees)\n", - "\n", - "#Result\n", - "print \"value of L is\",round(L,3),\"hbar\"\n", - "print \"value of S is\",round(S,3),\"hbar\"\n", - "print \"value of J for D5/2 state is\",round(J1,3),\"hbar\"\n", - "print \"value of J for D3/2 state is\",round(J2,3),\"hbar\"\n", - "print \"angle between L and S for D5/2 is\",round(theta1,2),\"degrees\"\n", - "print \"angle between L and S for D3/2 is\",int(theta2),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "value of L is 2.449 hbar\n", - "value of S is 0.866 hbar\n", - "value of J for D5/2 state is 2.958 hbar\n", - "value of J for D3/2 state is 1.936 hbar\n", - "angle between L and S for D5/2 is 61.87 degrees\n", - "angle between L and S for D3/2 is 135 degrees\n" - ] - } - ], - "prompt_number": 4 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.10, Page number 136" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "S=1;\n", - "L=1; \n", - "J=1;\n", - "\n", - "#Calculation\n", - "a=L*(L+1)-(L*(L+1));\n", - "g1=1+(a/(2*L*(L+1))); #lande's g-factor for pure orbital angular momentum\n", - "b=(S*(S+1)+(S*(S+1)))/(2*S*(S+1)); #lande's g-factor for pure spin angular momentum\n", - "g2=1+b; #lande's g-factor for pure spin angular momentum\n", - "c=J*(J+1)+(S*(S+1))-(L*(L+1));\n", - "g3=1+(c/(2*J*(J+1))); #lande's g-factor for state 3P1\n", - "\n", - "#Result\n", - "print \"lande's g-factor for pure orbital angular momentum is\",g1\n", - "print \"ande's g-factor for pure spin angular momentum is\",g2\n", - "print \"lande's g-factor for state 3P1 is\",g3" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "lande's g-factor for pure orbital angular momentum is 1.0\n", - "ande's g-factor for pure spin angular momentum is 2.0\n", - "lande's g-factor for state 3P1 is 1.5\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.12, Page number 141" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "EKalpha=21.99; #energy in silver(keV)\n", - "EKbita=25.145; #energy in silver(keV)\n", - "E=-25.514; #energy of n=1 state(keV)\n", - " \n", - "#Calculation\n", - "ELalpha=EKbita-EKalpha; #energy of L alpha X ray(keV)\n", - "E2=-E-EKalpha; #binding energy of L electron(keV)\n", - "\n", - "#Result\n", - "print \"energy of L alpha X ray is\",ELalpha,\"keV\"\n", - "print \"binding energy of L electron is\",E2,\"keV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy of L alpha X ray is 3.155 keV\n", - "binding energy of L electron is 3.524 keV\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.13, Page number 141" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "Z=11; #atomic number\n", - "R=1.097*10**7; #value of R(per m)\n", - "\n", - "#Calculation\n", - "E=(3*h*c*R*(Z-1)**2)/4; #energy of k aplha X-ray(keV)\n", - "\n", - "#Result\n", - "print \"energy of k aplha X-ray is\",round(E*10**16,2),\"*10**-16 keV\"\n", - "print \"answer given in the book is wrong\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy of k aplha X-ray is 1.64 *10**-16 keV\n", - "answer given in the book is wrong\n" - ] - } - ], - "prompt_number": 12 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter7_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter7_1.ipynb deleted file mode 100755 index 45ed5766..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter7_1.ipynb +++ /dev/null @@ -1,258 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:1e02050388cdd15ca19e058c38c307c0fd0b145ef71769674c045940ea70b08b" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "7: Atomic physics" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.1, Page number 113" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mewB=9.27*10**-24;\n", - "B=3; #magnetic field(T)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "E=2*mewB*B/e; #energy difference(eV)\n", - "\n", - "#Result\n", - "print \"energy difference is\",round(E*10**4,2),\"*10**-4 eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy difference is 3.48 *10**-4 eV\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.3, Page number 118" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "l=2;\n", - "s=1/2;\n", - "j1=2+(1/2);\n", - "j2=2-(1/2);\n", - "\n", - "#Calculation\n", - "L=math.sqrt(l*(l+1)); #value of L(hbar)\n", - "S=math.sqrt(s*(s+1)); #value of S(hbar)\n", - "J1=math.sqrt(j1*(j1+1)); #value of J for D5/2 state(hbar)\n", - "J2=math.sqrt(j2*(j2+1)); #value of J for D3/2 state(hbar)\n", - "costheta1=((j1*(j1+1))-(l*(l+1))-(s*(s+1)))/(2*L*S);\n", - "theta1=math.acos(costheta1); #angle between L and S for D5/2(radian)\n", - "theta1=theta1*180/math.pi; #angle between L and S for D5/2(degrees)\n", - "costheta2=((j2*(j2+1))-(l*(l+1))-(s*(s+1)))/(2*L*S);\n", - "theta2=math.acos(costheta2); #angle between L and S for D3/2(radian)\n", - "theta2=theta2*180/math.pi; #angle between L and S for D3/2(degrees)\n", - "\n", - "#Result\n", - "print \"value of L is\",round(L,3),\"hbar\"\n", - "print \"value of S is\",round(S,3),\"hbar\"\n", - "print \"value of J for D5/2 state is\",round(J1,3),\"hbar\"\n", - "print \"value of J for D3/2 state is\",round(J2,3),\"hbar\"\n", - "print \"angle between L and S for D5/2 is\",round(theta1,2),\"degrees\"\n", - "print \"angle between L and S for D3/2 is\",int(theta2),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "value of L is 2.449 hbar\n", - "value of S is 0.866 hbar\n", - "value of J for D5/2 state is 2.958 hbar\n", - "value of J for D3/2 state is 1.936 hbar\n", - "angle between L and S for D5/2 is 61.87 degrees\n", - "angle between L and S for D3/2 is 135 degrees\n" - ] - } - ], - "prompt_number": 4 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.10, Page number 136" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "S=1;\n", - "L=1; \n", - "J=1;\n", - "\n", - "#Calculation\n", - "a=L*(L+1)-(L*(L+1));\n", - "g1=1+(a/(2*L*(L+1))); #lande's g-factor for pure orbital angular momentum\n", - "b=(S*(S+1)+(S*(S+1)))/(2*S*(S+1)); #lande's g-factor for pure spin angular momentum\n", - "g2=1+b; #lande's g-factor for pure spin angular momentum\n", - "c=J*(J+1)+(S*(S+1))-(L*(L+1));\n", - "g3=1+(c/(2*J*(J+1))); #lande's g-factor for state 3P1\n", - "\n", - "#Result\n", - "print \"lande's g-factor for pure orbital angular momentum is\",g1\n", - "print \"ande's g-factor for pure spin angular momentum is\",g2\n", - "print \"lande's g-factor for state 3P1 is\",g3" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "lande's g-factor for pure orbital angular momentum is 1.0\n", - "ande's g-factor for pure spin angular momentum is 2.0\n", - "lande's g-factor for state 3P1 is 1.5\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.12, Page number 141" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "EKalpha=21.99; #energy in silver(keV)\n", - "EKbita=25.145; #energy in silver(keV)\n", - "E=-25.514; #energy of n=1 state(keV)\n", - " \n", - "#Calculation\n", - "ELalpha=EKbita-EKalpha; #energy of L alpha X ray(keV)\n", - "E2=-E-EKalpha; #binding energy of L electron(keV)\n", - "\n", - "#Result\n", - "print \"energy of L alpha X ray is\",ELalpha,\"keV\"\n", - "print \"binding energy of L electron is\",E2,\"keV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy of L alpha X ray is 3.155 keV\n", - "binding energy of L electron is 3.524 keV\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.13, Page number 141" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "Z=11; #atomic number\n", - "R=1.097*10**7; #value of R(per m)\n", - "\n", - "#Calculation\n", - "E=(3*h*c*R*(Z-1)**2)/4; #energy of k aplha X-ray(keV)\n", - "\n", - "#Result\n", - "print \"energy of k aplha X-ray is\",round(E*10**16,2),\"*10**-16 keV\"\n", - "print \"answer given in the book is wrong\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy of k aplha X-ray is 1.64 *10**-16 keV\n", - "answer given in the book is wrong\n" - ] - } - ], - "prompt_number": 12 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter7_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter7_2.ipynb deleted file mode 100755 index 45ed5766..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter7_2.ipynb +++ /dev/null @@ -1,258 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:1e02050388cdd15ca19e058c38c307c0fd0b145ef71769674c045940ea70b08b" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "7: Atomic physics" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.1, Page number 113" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "mewB=9.27*10**-24;\n", - "B=3; #magnetic field(T)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "E=2*mewB*B/e; #energy difference(eV)\n", - "\n", - "#Result\n", - "print \"energy difference is\",round(E*10**4,2),\"*10**-4 eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy difference is 3.48 *10**-4 eV\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.3, Page number 118" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "l=2;\n", - "s=1/2;\n", - "j1=2+(1/2);\n", - "j2=2-(1/2);\n", - "\n", - "#Calculation\n", - "L=math.sqrt(l*(l+1)); #value of L(hbar)\n", - "S=math.sqrt(s*(s+1)); #value of S(hbar)\n", - "J1=math.sqrt(j1*(j1+1)); #value of J for D5/2 state(hbar)\n", - "J2=math.sqrt(j2*(j2+1)); #value of J for D3/2 state(hbar)\n", - "costheta1=((j1*(j1+1))-(l*(l+1))-(s*(s+1)))/(2*L*S);\n", - "theta1=math.acos(costheta1); #angle between L and S for D5/2(radian)\n", - "theta1=theta1*180/math.pi; #angle between L and S for D5/2(degrees)\n", - "costheta2=((j2*(j2+1))-(l*(l+1))-(s*(s+1)))/(2*L*S);\n", - "theta2=math.acos(costheta2); #angle between L and S for D3/2(radian)\n", - "theta2=theta2*180/math.pi; #angle between L and S for D3/2(degrees)\n", - "\n", - "#Result\n", - "print \"value of L is\",round(L,3),\"hbar\"\n", - "print \"value of S is\",round(S,3),\"hbar\"\n", - "print \"value of J for D5/2 state is\",round(J1,3),\"hbar\"\n", - "print \"value of J for D3/2 state is\",round(J2,3),\"hbar\"\n", - "print \"angle between L and S for D5/2 is\",round(theta1,2),\"degrees\"\n", - "print \"angle between L and S for D3/2 is\",int(theta2),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "value of L is 2.449 hbar\n", - "value of S is 0.866 hbar\n", - "value of J for D5/2 state is 2.958 hbar\n", - "value of J for D3/2 state is 1.936 hbar\n", - "angle between L and S for D5/2 is 61.87 degrees\n", - "angle between L and S for D3/2 is 135 degrees\n" - ] - } - ], - "prompt_number": 4 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.10, Page number 136" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "S=1;\n", - "L=1; \n", - "J=1;\n", - "\n", - "#Calculation\n", - "a=L*(L+1)-(L*(L+1));\n", - "g1=1+(a/(2*L*(L+1))); #lande's g-factor for pure orbital angular momentum\n", - "b=(S*(S+1)+(S*(S+1)))/(2*S*(S+1)); #lande's g-factor for pure spin angular momentum\n", - "g2=1+b; #lande's g-factor for pure spin angular momentum\n", - "c=J*(J+1)+(S*(S+1))-(L*(L+1));\n", - "g3=1+(c/(2*J*(J+1))); #lande's g-factor for state 3P1\n", - "\n", - "#Result\n", - "print \"lande's g-factor for pure orbital angular momentum is\",g1\n", - "print \"ande's g-factor for pure spin angular momentum is\",g2\n", - "print \"lande's g-factor for state 3P1 is\",g3" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "lande's g-factor for pure orbital angular momentum is 1.0\n", - "ande's g-factor for pure spin angular momentum is 2.0\n", - "lande's g-factor for state 3P1 is 1.5\n" - ] - } - ], - "prompt_number": 6 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.12, Page number 141" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "EKalpha=21.99; #energy in silver(keV)\n", - "EKbita=25.145; #energy in silver(keV)\n", - "E=-25.514; #energy of n=1 state(keV)\n", - " \n", - "#Calculation\n", - "ELalpha=EKbita-EKalpha; #energy of L alpha X ray(keV)\n", - "E2=-E-EKalpha; #binding energy of L electron(keV)\n", - "\n", - "#Result\n", - "print \"energy of L alpha X ray is\",ELalpha,\"keV\"\n", - "print \"binding energy of L electron is\",E2,\"keV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy of L alpha X ray is 3.155 keV\n", - "binding energy of L electron is 3.524 keV\n" - ] - } - ], - "prompt_number": 8 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 7.13, Page number 141" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "Z=11; #atomic number\n", - "R=1.097*10**7; #value of R(per m)\n", - "\n", - "#Calculation\n", - "E=(3*h*c*R*(Z-1)**2)/4; #energy of k aplha X-ray(keV)\n", - "\n", - "#Result\n", - "print \"energy of k aplha X-ray is\",round(E*10**16,2),\"*10**-16 keV\"\n", - "print \"answer given in the book is wrong\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "energy of k aplha X-ray is 1.64 *10**-16 keV\n", - "answer given in the book is wrong\n" - ] - } - ], - "prompt_number": 12 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter8.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter8.ipynb deleted file mode 100755 index 014cb0d9..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter8.ipynb +++ /dev/null @@ -1,116 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:3bf1b2120b5dacb9d86b4fa6efbc4300ebec3d48ce95ec80e2e6a8f936088a09" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "8: Statistical physics" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 8.2, Page number 164" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "rho=10.5; #density of silver(g/cc)\n", - "M=108; #atomic weight(g/mole)\n", - "NA=6.02*10**23; #avagadro number(atoms/mole)\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "NbyV=rho*NA/M; #number density of conduction electrons(per cc)\n", - "NbyV=NbyV*10**6; #number density of conduction electrons(per m**3)\n", - "EF=(h**2/(8*m))*(3*NbyV/math.pi)**(2/3); #fermi energy(J)\n", - "EF=EF/e; #fermi energy(eV)\n", - "E=3*EF/5; #mean energy of electron(eV)\n", - "\n", - "#Result\n", - "print \"number density of conduction electrons is\",round(NbyV/10**28,2),\"*10**28 per m**3\"\n", - "print \"fermi energy is\",round(EF,2),\"eV\"\n", - "print \"mean energy of electron is\",round(E,2),\"eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number density of conduction electrons is 5.85 *10**28 per m**3\n", - "fermi energy is 5.51 eV\n", - "mean energy of electron is 3.31 eV\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 8.3, Page number 164" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "T=300; #temperature(K)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "EF=5.49; #fermi energy(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "R=1; #assume\n", - "\n", - "#Calculation\n", - "CV=math.pi**2*k*T*R/(2*EF*e); #electronic contribution of Silver(R)\n", - "\n", - "#Result\n", - "print \"electronic contribution of Silver is\",round(CV,5),\"R\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "electronic contribution of Silver is 0.02326 R\n" - ] - } - ], - "prompt_number": 9 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter8_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter8_1.ipynb deleted file mode 100755 index 014cb0d9..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter8_1.ipynb +++ /dev/null @@ -1,116 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:3bf1b2120b5dacb9d86b4fa6efbc4300ebec3d48ce95ec80e2e6a8f936088a09" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "8: Statistical physics" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 8.2, Page number 164" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "rho=10.5; #density of silver(g/cc)\n", - "M=108; #atomic weight(g/mole)\n", - "NA=6.02*10**23; #avagadro number(atoms/mole)\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "NbyV=rho*NA/M; #number density of conduction electrons(per cc)\n", - "NbyV=NbyV*10**6; #number density of conduction electrons(per m**3)\n", - "EF=(h**2/(8*m))*(3*NbyV/math.pi)**(2/3); #fermi energy(J)\n", - "EF=EF/e; #fermi energy(eV)\n", - "E=3*EF/5; #mean energy of electron(eV)\n", - "\n", - "#Result\n", - "print \"number density of conduction electrons is\",round(NbyV/10**28,2),\"*10**28 per m**3\"\n", - "print \"fermi energy is\",round(EF,2),\"eV\"\n", - "print \"mean energy of electron is\",round(E,2),\"eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number density of conduction electrons is 5.85 *10**28 per m**3\n", - "fermi energy is 5.51 eV\n", - "mean energy of electron is 3.31 eV\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 8.3, Page number 164" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "T=300; #temperature(K)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "EF=5.49; #fermi energy(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "R=1; #assume\n", - "\n", - "#Calculation\n", - "CV=math.pi**2*k*T*R/(2*EF*e); #electronic contribution of Silver(R)\n", - "\n", - "#Result\n", - "print \"electronic contribution of Silver is\",round(CV,5),\"R\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "electronic contribution of Silver is 0.02326 R\n" - ] - } - ], - "prompt_number": 9 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter8_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter8_2.ipynb deleted file mode 100755 index 014cb0d9..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter8_2.ipynb +++ /dev/null @@ -1,116 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:3bf1b2120b5dacb9d86b4fa6efbc4300ebec3d48ce95ec80e2e6a8f936088a09" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "8: Statistical physics" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 8.2, Page number 164" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "rho=10.5; #density of silver(g/cc)\n", - "M=108; #atomic weight(g/mole)\n", - "NA=6.02*10**23; #avagadro number(atoms/mole)\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "m=9.1*10**-31; #mass of electron(kg)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "\n", - "#Calculation\n", - "NbyV=rho*NA/M; #number density of conduction electrons(per cc)\n", - "NbyV=NbyV*10**6; #number density of conduction electrons(per m**3)\n", - "EF=(h**2/(8*m))*(3*NbyV/math.pi)**(2/3); #fermi energy(J)\n", - "EF=EF/e; #fermi energy(eV)\n", - "E=3*EF/5; #mean energy of electron(eV)\n", - "\n", - "#Result\n", - "print \"number density of conduction electrons is\",round(NbyV/10**28,2),\"*10**28 per m**3\"\n", - "print \"fermi energy is\",round(EF,2),\"eV\"\n", - "print \"mean energy of electron is\",round(E,2),\"eV\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "number density of conduction electrons is 5.85 *10**28 per m**3\n", - "fermi energy is 5.51 eV\n", - "mean energy of electron is 3.31 eV\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 8.3, Page number 164" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "T=300; #temperature(K)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "EF=5.49; #fermi energy(eV)\n", - "e=1.6*10**-19; #conversion factor from J to eV\n", - "R=1; #assume\n", - "\n", - "#Calculation\n", - "CV=math.pi**2*k*T*R/(2*EF*e); #electronic contribution of Silver(R)\n", - "\n", - "#Result\n", - "print \"electronic contribution of Silver is\",round(CV,5),\"R\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "electronic contribution of Silver is 0.02326 R\n" - ] - } - ], - "prompt_number": 9 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter9.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter9.ipynb deleted file mode 100755 index fa1ac5e9..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter9.ipynb +++ /dev/null @@ -1,418 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:d1e925900cff60559a1ba3f62c2c267140215c90675c4dba42b1a473becca175" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "9: Molecular spectra" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.1, Page number 172" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "twoB=3.8626; #average spacing(per cm)\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #speed of light(m/s)\n", - "NA=6.022*10**23; #avagadro number(atoms/mole)\n", - "mC=0.012; #isotopic mass of C(kg/mol)\n", - "mO=0.016; #isotopic mass of O(kg/mol)\n", - "\n", - "#Calculation\n", - "B=(twoB/2)*100; #average spacing(per m)\n", - "I=h/(8*math.pi**2*B*c); \n", - "mew=mC*mO/((mC+mO)*NA); #reduced mass(kg)\n", - "r=math.sqrt(I/mew); #bond length(m)\n", - "\n", - "#Result\n", - "print \"bond length is\",round(r*10**10,3),\"*10**-10 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "bond length is 1.128 *10**-10 m\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.2, Page number 173" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "T=300; #temperature(K)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #speed of light(m/s)\n", - "lamda=10**-2; #wavelength(m)\n", - "\n", - "#Calculation\n", - "E=3*k*T/2; #kinetic energy(J)\n", - "deltaE=h*c/lamda; #energy seperation(J)\n", - "\n", - "#Result\n", - "print \"kinetic energy is\",E,\"J\"\n", - "print \"energy seperation is\",round(deltaE*10**23),\"*10**-23 J\"\n", - "print \"deltaE is much smaller than E. hence substantial number of molecules will be there\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "kinetic energy is 6.21e-21 J\n", - "energy seperation is 2.0 *10**-23 J\n", - "deltaE is much smaller than E. hence substantial number of molecules will be there\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.3, Page number 175" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "ff=1876.06; #frequency of fundamental(per cm)\n", - "fo=3724.2; #frequency of 1st overtone(per cm)\n", - "\n", - "#Calculation\n", - "#ff=vebar*(1-(2*xe)) and fo=2*vebar*(1-(3*xe)). on solcing we get\n", - "vebar=1903.98; #equilibrium vibration frequency(per cm)\n", - "xe=7.33*10**-3; #anharmonicity constant\n", - "E=vebar/2; #zero point energy(per cm)\n", - "\n", - "#Result\n", - "print \"equilibrium vibration frequency is\",vebar,\"per cm\"\n", - "print \"anharmonicity constant is\",round(xe*10**3,2),\"*10**-3\"\n", - "print \"zero point energy is\",round(E),\"per cm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "equilibrium vibration frequency is 1903.98 per cm\n", - "anharmonicity constant is 7.33 *10**-3\n", - "zero point energy is 952.0 per cm\n" - ] - } - ], - "prompt_number": 10 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.4, Page number 175" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m=1.67*10**-27; #mass of proton(kg)\n", - "m1=1.0087; #mass of 1H(u)\n", - "m2=35.453; #mass of Cl(u)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda0=3.465*10**-6; #wavelength(m)\n", - "\n", - "#Calculation\n", - "mew=m*m1*m2/(m1+m2); #reduced mass(kg)\n", - "k=4*math.pi**2*mew*(c/lamda0)**2; #force constant(N/m)\n", - "\n", - "#Result\n", - "print \"force constant is\",round(k,1),\"N/m\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "force constant is 484.7 N/m\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.5, Page number 187" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamdae=4358.3*10**-8; #excited wavelength(cm)\n", - "lamda=4768.5*10**-8; #wavelength(cm)\n", - "\n", - "#Calculation\n", - "wne=1/lamdae; #wave number of exciting radiation(per cm)\n", - "wn=1/lamda; #wave number of Raman line(per cm)\n", - "new=wne-wn; #vibrational frequency(per cm)\n", - "\n", - "#Result\n", - "print \"vibrational frequency is\",round(new),\"per cm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "vibrational frequency is 1974.0 per cm\n" - ] - } - ], - "prompt_number": 15 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.6, Page number 188" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #speed of light(m/s)\n", - "sixB=346; #1st rotational Raman line(per cm)\n", - "m1=1.673*10**-27; #mass of proton(kg)\n", - "\n", - "#Calculation\n", - "m2=m1;\n", - "B=(sixB/6)*100; #average spacing(per m)\n", - "I=h/(8*math.pi**2*B*c); \n", - "mew=m1*m2/(m1+m2); #reduced mass(kg)\n", - "r=math.sqrt(I/mew); #bond length(m)\n", - "\n", - "#Result\n", - "print \"bond length is\",round(r*10**10,3),\"*10**-10 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "bond length is 0.762 *10**-10 m\n" - ] - } - ], - "prompt_number": 18 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.7, Page number 193" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "gN=5.585; #value of gN\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new=120*10**6; #frequency(Hz)\n", - "mewn=5.0508*10**-27;\n", - "\n", - "#Calculation\n", - "B0=h*new/(gN*mewn); #magnetic field strength(T)\n", - "\n", - "#Result\n", - "print \"magnetic field strength is\",round(B0,3),\"T\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "magnetic field strength is 2.819 T\n" - ] - } - ], - "prompt_number": 20 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.8, Page number 194" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "gN=5.585; #value of gN\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "mewn=5.0508*10**-27;\n", - "B0=1.65; #magnetic field(T)\n", - "new=510*10**6; #frequency separation(Hz)\n", - "\n", - "#Calculation\n", - "new0=gN*mewn*B0/h;\n", - "delta=new/new0; #chemical shift(ppm)\n", - "\n", - "#Result\n", - "print \"chemical shift is\",round(delta,2),\"ppm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "chemical shift is 7.26 ppm\n" - ] - } - ], - "prompt_number": 24 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.10, Page number 198" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new=35*10**9; #frequency(Hz)\n", - "mewB=9.27*10**-24;\n", - "B0=1.3; #magnetic field(T)\n", - "\n", - "#Calculation\n", - "g=h*new/(mewB*B0); #electron g-factor\n", - "\n", - "#Result\n", - "print \"electron g-factor is\",round(g,3)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "electron g-factor is 1.924\n" - ] - } - ], - "prompt_number": 26 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter9_1.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter9_1.ipynb deleted file mode 100755 index fa1ac5e9..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter9_1.ipynb +++ /dev/null @@ -1,418 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:d1e925900cff60559a1ba3f62c2c267140215c90675c4dba42b1a473becca175" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "9: Molecular spectra" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.1, Page number 172" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "twoB=3.8626; #average spacing(per cm)\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #speed of light(m/s)\n", - "NA=6.022*10**23; #avagadro number(atoms/mole)\n", - "mC=0.012; #isotopic mass of C(kg/mol)\n", - "mO=0.016; #isotopic mass of O(kg/mol)\n", - "\n", - "#Calculation\n", - "B=(twoB/2)*100; #average spacing(per m)\n", - "I=h/(8*math.pi**2*B*c); \n", - "mew=mC*mO/((mC+mO)*NA); #reduced mass(kg)\n", - "r=math.sqrt(I/mew); #bond length(m)\n", - "\n", - "#Result\n", - "print \"bond length is\",round(r*10**10,3),\"*10**-10 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "bond length is 1.128 *10**-10 m\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.2, Page number 173" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "T=300; #temperature(K)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #speed of light(m/s)\n", - "lamda=10**-2; #wavelength(m)\n", - "\n", - "#Calculation\n", - "E=3*k*T/2; #kinetic energy(J)\n", - "deltaE=h*c/lamda; #energy seperation(J)\n", - "\n", - "#Result\n", - "print \"kinetic energy is\",E,\"J\"\n", - "print \"energy seperation is\",round(deltaE*10**23),\"*10**-23 J\"\n", - "print \"deltaE is much smaller than E. hence substantial number of molecules will be there\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "kinetic energy is 6.21e-21 J\n", - "energy seperation is 2.0 *10**-23 J\n", - "deltaE is much smaller than E. hence substantial number of molecules will be there\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.3, Page number 175" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "ff=1876.06; #frequency of fundamental(per cm)\n", - "fo=3724.2; #frequency of 1st overtone(per cm)\n", - "\n", - "#Calculation\n", - "#ff=vebar*(1-(2*xe)) and fo=2*vebar*(1-(3*xe)). on solcing we get\n", - "vebar=1903.98; #equilibrium vibration frequency(per cm)\n", - "xe=7.33*10**-3; #anharmonicity constant\n", - "E=vebar/2; #zero point energy(per cm)\n", - "\n", - "#Result\n", - "print \"equilibrium vibration frequency is\",vebar,\"per cm\"\n", - "print \"anharmonicity constant is\",round(xe*10**3,2),\"*10**-3\"\n", - "print \"zero point energy is\",round(E),\"per cm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "equilibrium vibration frequency is 1903.98 per cm\n", - "anharmonicity constant is 7.33 *10**-3\n", - "zero point energy is 952.0 per cm\n" - ] - } - ], - "prompt_number": 10 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.4, Page number 175" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m=1.67*10**-27; #mass of proton(kg)\n", - "m1=1.0087; #mass of 1H(u)\n", - "m2=35.453; #mass of Cl(u)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda0=3.465*10**-6; #wavelength(m)\n", - "\n", - "#Calculation\n", - "mew=m*m1*m2/(m1+m2); #reduced mass(kg)\n", - "k=4*math.pi**2*mew*(c/lamda0)**2; #force constant(N/m)\n", - "\n", - "#Result\n", - "print \"force constant is\",round(k,1),\"N/m\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "force constant is 484.7 N/m\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.5, Page number 187" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamdae=4358.3*10**-8; #excited wavelength(cm)\n", - "lamda=4768.5*10**-8; #wavelength(cm)\n", - "\n", - "#Calculation\n", - "wne=1/lamdae; #wave number of exciting radiation(per cm)\n", - "wn=1/lamda; #wave number of Raman line(per cm)\n", - "new=wne-wn; #vibrational frequency(per cm)\n", - "\n", - "#Result\n", - "print \"vibrational frequency is\",round(new),\"per cm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "vibrational frequency is 1974.0 per cm\n" - ] - } - ], - "prompt_number": 15 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.6, Page number 188" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #speed of light(m/s)\n", - "sixB=346; #1st rotational Raman line(per cm)\n", - "m1=1.673*10**-27; #mass of proton(kg)\n", - "\n", - "#Calculation\n", - "m2=m1;\n", - "B=(sixB/6)*100; #average spacing(per m)\n", - "I=h/(8*math.pi**2*B*c); \n", - "mew=m1*m2/(m1+m2); #reduced mass(kg)\n", - "r=math.sqrt(I/mew); #bond length(m)\n", - "\n", - "#Result\n", - "print \"bond length is\",round(r*10**10,3),\"*10**-10 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "bond length is 0.762 *10**-10 m\n" - ] - } - ], - "prompt_number": 18 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.7, Page number 193" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "gN=5.585; #value of gN\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new=120*10**6; #frequency(Hz)\n", - "mewn=5.0508*10**-27;\n", - "\n", - "#Calculation\n", - "B0=h*new/(gN*mewn); #magnetic field strength(T)\n", - "\n", - "#Result\n", - "print \"magnetic field strength is\",round(B0,3),\"T\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "magnetic field strength is 2.819 T\n" - ] - } - ], - "prompt_number": 20 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.8, Page number 194" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "gN=5.585; #value of gN\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "mewn=5.0508*10**-27;\n", - "B0=1.65; #magnetic field(T)\n", - "new=510*10**6; #frequency separation(Hz)\n", - "\n", - "#Calculation\n", - "new0=gN*mewn*B0/h;\n", - "delta=new/new0; #chemical shift(ppm)\n", - "\n", - "#Result\n", - "print \"chemical shift is\",round(delta,2),\"ppm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "chemical shift is 7.26 ppm\n" - ] - } - ], - "prompt_number": 24 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.10, Page number 198" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new=35*10**9; #frequency(Hz)\n", - "mewB=9.27*10**-24;\n", - "B0=1.3; #magnetic field(T)\n", - "\n", - "#Calculation\n", - "g=h*new/(mewB*B0); #electron g-factor\n", - "\n", - "#Result\n", - "print \"electron g-factor is\",round(g,3)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "electron g-factor is 1.924\n" - ] - } - ], - "prompt_number": 26 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file diff --git a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter9_2.ipynb b/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter9_2.ipynb deleted file mode 100755 index fa1ac5e9..00000000 --- a/backup/Modern_Physics_By_G.Aruldas_version_backup/Chapter9_2.ipynb +++ /dev/null @@ -1,418 +0,0 @@ -{ - "metadata": { - "name": "", - "signature": "sha256:d1e925900cff60559a1ba3f62c2c267140215c90675c4dba42b1a473becca175" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "9: Molecular spectra" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.1, Page number 172" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "twoB=3.8626; #average spacing(per cm)\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #speed of light(m/s)\n", - "NA=6.022*10**23; #avagadro number(atoms/mole)\n", - "mC=0.012; #isotopic mass of C(kg/mol)\n", - "mO=0.016; #isotopic mass of O(kg/mol)\n", - "\n", - "#Calculation\n", - "B=(twoB/2)*100; #average spacing(per m)\n", - "I=h/(8*math.pi**2*B*c); \n", - "mew=mC*mO/((mC+mO)*NA); #reduced mass(kg)\n", - "r=math.sqrt(I/mew); #bond length(m)\n", - "\n", - "#Result\n", - "print \"bond length is\",round(r*10**10,3),\"*10**-10 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "bond length is 1.128 *10**-10 m\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.2, Page number 173" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "T=300; #temperature(K)\n", - "k=1.38*10**-23; #boltzmann constant(J/K)\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #speed of light(m/s)\n", - "lamda=10**-2; #wavelength(m)\n", - "\n", - "#Calculation\n", - "E=3*k*T/2; #kinetic energy(J)\n", - "deltaE=h*c/lamda; #energy seperation(J)\n", - "\n", - "#Result\n", - "print \"kinetic energy is\",E,\"J\"\n", - "print \"energy seperation is\",round(deltaE*10**23),\"*10**-23 J\"\n", - "print \"deltaE is much smaller than E. hence substantial number of molecules will be there\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "kinetic energy is 6.21e-21 J\n", - "energy seperation is 2.0 *10**-23 J\n", - "deltaE is much smaller than E. hence substantial number of molecules will be there\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.3, Page number 175" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "ff=1876.06; #frequency of fundamental(per cm)\n", - "fo=3724.2; #frequency of 1st overtone(per cm)\n", - "\n", - "#Calculation\n", - "#ff=vebar*(1-(2*xe)) and fo=2*vebar*(1-(3*xe)). on solcing we get\n", - "vebar=1903.98; #equilibrium vibration frequency(per cm)\n", - "xe=7.33*10**-3; #anharmonicity constant\n", - "E=vebar/2; #zero point energy(per cm)\n", - "\n", - "#Result\n", - "print \"equilibrium vibration frequency is\",vebar,\"per cm\"\n", - "print \"anharmonicity constant is\",round(xe*10**3,2),\"*10**-3\"\n", - "print \"zero point energy is\",round(E),\"per cm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "equilibrium vibration frequency is 1903.98 per cm\n", - "anharmonicity constant is 7.33 *10**-3\n", - "zero point energy is 952.0 per cm\n" - ] - } - ], - "prompt_number": 10 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.4, Page number 175" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m=1.67*10**-27; #mass of proton(kg)\n", - "m1=1.0087; #mass of 1H(u)\n", - "m2=35.453; #mass of Cl(u)\n", - "c=3*10**8; #velocity of light(m/sec)\n", - "lamda0=3.465*10**-6; #wavelength(m)\n", - "\n", - "#Calculation\n", - "mew=m*m1*m2/(m1+m2); #reduced mass(kg)\n", - "k=4*math.pi**2*mew*(c/lamda0)**2; #force constant(N/m)\n", - "\n", - "#Result\n", - "print \"force constant is\",round(k,1),\"N/m\"\n", - "print \"answer varies due to rounding off errors\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "force constant is 484.7 N/m\n", - "answer varies due to rounding off errors\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.5, Page number 187" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "lamdae=4358.3*10**-8; #excited wavelength(cm)\n", - "lamda=4768.5*10**-8; #wavelength(cm)\n", - "\n", - "#Calculation\n", - "wne=1/lamdae; #wave number of exciting radiation(per cm)\n", - "wn=1/lamda; #wave number of Raman line(per cm)\n", - "new=wne-wn; #vibrational frequency(per cm)\n", - "\n", - "#Result\n", - "print \"vibrational frequency is\",round(new),\"per cm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "vibrational frequency is 1974.0 per cm\n" - ] - } - ], - "prompt_number": 15 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.6, Page number 188" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "c=3*10**8; #speed of light(m/s)\n", - "sixB=346; #1st rotational Raman line(per cm)\n", - "m1=1.673*10**-27; #mass of proton(kg)\n", - "\n", - "#Calculation\n", - "m2=m1;\n", - "B=(sixB/6)*100; #average spacing(per m)\n", - "I=h/(8*math.pi**2*B*c); \n", - "mew=m1*m2/(m1+m2); #reduced mass(kg)\n", - "r=math.sqrt(I/mew); #bond length(m)\n", - "\n", - "#Result\n", - "print \"bond length is\",round(r*10**10,3),\"*10**-10 m\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "bond length is 0.762 *10**-10 m\n" - ] - } - ], - "prompt_number": 18 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.7, Page number 193" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "gN=5.585; #value of gN\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new=120*10**6; #frequency(Hz)\n", - "mewn=5.0508*10**-27;\n", - "\n", - "#Calculation\n", - "B0=h*new/(gN*mewn); #magnetic field strength(T)\n", - "\n", - "#Result\n", - "print \"magnetic field strength is\",round(B0,3),\"T\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "magnetic field strength is 2.819 T\n" - ] - } - ], - "prompt_number": 20 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.8, Page number 194" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "gN=5.585; #value of gN\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "mewn=5.0508*10**-27;\n", - "B0=1.65; #magnetic field(T)\n", - "new=510*10**6; #frequency separation(Hz)\n", - "\n", - "#Calculation\n", - "new0=gN*mewn*B0/h;\n", - "delta=new/new0; #chemical shift(ppm)\n", - "\n", - "#Result\n", - "print \"chemical shift is\",round(delta,2),\"ppm\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "chemical shift is 7.26 ppm\n" - ] - } - ], - "prompt_number": 24 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example number 9.10, Page number 198" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "h=6.626*10**-34; #planck's constant(Js)\n", - "new=35*10**9; #frequency(Hz)\n", - "mewB=9.27*10**-24;\n", - "B0=1.3; #magnetic field(T)\n", - "\n", - "#Calculation\n", - "g=h*new/(mewB*B0); #electron g-factor\n", - "\n", - "#Result\n", - "print \"electron g-factor is\",round(g,3)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "electron g-factor is 1.924\n" - ] - } - ], - "prompt_number": 26 - } - ], - "metadata": {} - } - ] -} \ No newline at end of file -- cgit