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diff --git a/Solid_State_Physics_by_Dr._M._Arumugam/Chapter6_wKefPQQ.ipynb b/Solid_State_Physics_by_Dr._M._Arumugam/Chapter6_wKefPQQ.ipynb deleted file mode 100644 index ab8cdc23..00000000 --- a/Solid_State_Physics_by_Dr._M._Arumugam/Chapter6_wKefPQQ.ipynb +++ /dev/null @@ -1,331 +0,0 @@ -{ - "cells": [ - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "# 6: Principles of Quantum Mechanics" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example number 1, Page number 6.22" - ] - }, - { - "cell_type": "code", - "execution_count": 2, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "deBroglie wavelength is 0.66 angstrom\n", - "spacing between planes is 0.35 angstrom\n" - ] - } - ], - "source": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "V=344; #voltage(V)\n", - "theta=40; #angle(degrees)\n", - "n=1; \n", - "\n", - "#Calculation\n", - "lamda=12.26/math.sqrt(V); #deBroglie wavelength(angstrom)\n", - "theta=((180-theta)/2)*math.pi/180; #angle(radian)\n", - "d=n*lamda/(2*math.sin(theta)); #spacing between planes(angstrom)\n", - "\n", - "#Result\n", - "print \"deBroglie wavelength is\",round(lamda,2),\"angstrom\"\n", - "print \"spacing between planes is\",round(d,2),\"angstrom\"" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example number 2, Page number 6.22" - ] - }, - { - "cell_type": "code", - "execution_count": 6, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "deBroglie wavelength is 0.00286 angstrom\n" - ] - } - ], - "source": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #charge(coulomb)\n", - "m=1.675*10**-27; #mass(kg)\n", - "E=10*10**3*e; #kinetic energy(J)\n", - "h=6.625*10**-34; #planks constant(Js)\n", - "\n", - "#Calculation\n", - "v=math.sqrt(2*E/m); #velocity(m/sec)\n", - "lamda=h*10**10/(m*v); #deBroglie wavelength(angstrom)\n", - "\n", - "#Result\n", - "print \"deBroglie wavelength is\",round(lamda,5),\"angstrom\"" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example number 3, Page number 6.22" - ] - }, - { - "cell_type": "code", - "execution_count": 8, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "energy difference is 1.81 *10**-37 J\n" - ] - } - ], - "source": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m=9.1*10**-31; #mass(kg)\n", - "h=6.63*10**-34; #planks constant(Js)\n", - "a=1; #length(m)\n", - "nx1=1;\n", - "ny1=1;\n", - "nz1=1;\n", - "nx2=1;\n", - "ny2=1;\n", - "nz2=2;\n", - "\n", - "#Calculation\n", - "E1=h**2*(nx1**2+ny1**2+nz1**2)/(8*m*a**2); #energy of 1st quantum state(J)\n", - "E2=h**2*(nx2**2+ny2**2+nz2**2)/(8*m*a**2); #energy of 2nd quantum state(J)\n", - "E=E2-E1; #energy difference(J)\n", - "\n", - "#Result\n", - "print \"energy difference is\",round(E*10**37,2),\"*10**-37 J\"" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example number 4, Page number 6.23" - ] - }, - { - "cell_type": "code", - "execution_count": 12, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "uncertainity in position of electron is 0.002 m\n", - "uncertainity in position of bullet is 0.4 *10**-31 m\n" - ] - } - ], - "source": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "m1=9.1*10**-31; #mass(kg)\n", - "m2=0.05; #mass(kg)\n", - "v=300; #velocity(m/sec)\n", - "p=0.01/100; #probability\n", - "h=6.6*10**-34; #planks constant(Js)\n", - "\n", - "#Calculation\n", - "p1=m1*v; #momentum of electron(kg m/s)\n", - "deltap1=p*p1; \n", - "deltax1=h/(deltap1*4*math.pi); #uncertainity in position of electron(m)\n", - "p2=m2*v; #momentum of bullet(kg m/s)\n", - "deltap2=p*p2; \n", - "deltax2=h/(deltap2*4*math.pi); #uncertainity in position of bullet(m)\n", - "\n", - "#Result\n", - "print \"uncertainity in position of electron is\",round(deltax1,3),\"m\"\n", - "print \"uncertainity in position of bullet is\",round(deltax2*10**31,1),\"*10**-31 m\"" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example number 5, Page number 6.24" - ] - }, - { - "cell_type": "code", - "execution_count": 13, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "probability of finding the particle is 0.2\n" - ] - } - ], - "source": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "deltax=10**-10; #uncertainity in position(m)\n", - "L=10*10**-10; #width(m)\n", - "\n", - "#Calculation\n", - "p=2*deltax/L; #probability of finding the particle\n", - "\n", - "#Result\n", - "print \"probability of finding the particle is\",p" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example number 6, Page number 6.24" - ] - }, - { - "cell_type": "code", - "execution_count": 15, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "deBroglie wavelength is 2.73 *10**-11 m\n" - ] - } - ], - "source": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.6*10**-19; #charge(coulomb)\n", - "m=9.1*10**-31; #mass(kg)\n", - "E=2*10**3*e; #kinetic energy(J)\n", - "h=6.6*10**-34; #planks constant(Js)\n", - "\n", - "#Calculation\n", - "p=math.sqrt(2*E*m); #momentum(kg m/s)\n", - "lamda=h/p; #deBroglie wavelength(m)\n", - "\n", - "#Result\n", - "print \"deBroglie wavelength is\",round(lamda*10**11,2),\"*10**-11 m\"" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example number 7, Page number 6.24" - ] - }, - { - "cell_type": "code", - "execution_count": 21, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "deBroglie wavelength is 1.807 angstrom\n" - ] - } - ], - "source": [ - "#importing modules\n", - "import math\n", - "from __future__ import division\n", - "\n", - "#Variable declaration\n", - "e=1.602*10**-19; #charge(coulomb)\n", - "m=1.676*10**-27; #mass(kg)\n", - "h=6.62*10**-34; #planks constant(Js)\n", - "E=0.025*e; #kinetic energy(J)\n", - "\n", - "#Calculation\n", - "mv=math.sqrt(2*E*m); #velocity(m/s)\n", - "lamda=h*10**10/mv; #deBroglie wavelength(angstrom)\n", - "\n", - "#Result\n", - "print \"deBroglie wavelength is\",round(lamda,3),\"angstrom\"" - ] - } - ], - "metadata": { - "kernelspec": { - "display_name": "Python 2", - "language": "python", - "name": "python2" - }, - "language_info": { - "codemirror_mode": { - "name": "ipython", - "version": 2 - }, - "file_extension": ".py", - "mimetype": "text/x-python", - "name": "python", - "nbconvert_exporter": "python", - "pygments_lexer": "ipython2", - "version": "2.7.11" - } - }, - "nbformat": 4, - "nbformat_minor": 0 -} |