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author | kinitrupti | 2017-05-12 18:40:35 +0530 |
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committer | kinitrupti | 2017-05-12 18:40:35 +0530 |
commit | d36fc3b8f88cc3108ffff6151e376b619b9abb01 (patch) | |
tree | 9806b0d68a708d2cfc4efc8ae3751423c56b7721 /Modern_Physics_By_G.Aruldas/Chapter10_2.ipynb | |
parent | 1b1bb67e9ea912be5c8591523c8b328766e3680f (diff) | |
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diff --git a/Modern_Physics_By_G.Aruldas/Chapter10_2.ipynb b/Modern_Physics_By_G.Aruldas/Chapter10_2.ipynb deleted file mode 100755 index d4104917..00000000 --- a/Modern_Physics_By_G.Aruldas/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": {}
- }
- ]
-}
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