{ "cells": [ { "cell_type": "markdown", "metadata": {}, "source": [ "# 6: Principles of quantum mechanics" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.1, Page number 6.8" ] }, { "cell_type": "code", "execution_count": 4, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "de broglie wavelength is 1.323 *10**-14 m\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "c=3*10**8; #velocity of light(m/s)\n", "m=1.67*10**-27; #mass of proton(kg)\n", "h=6.626*10**-34; #planck's constant\n", "\n", "#Calculation\n", "lamda=h*10/(m*c); #de broglie wavelength(m)\n", "\n", "#Result\n", "print \"de broglie wavelength is\",round(lamda*10**14,3),\"*10**-14 m\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.2, Page number 6.8" ] }, { "cell_type": "code", "execution_count": 6, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "de broglie wavelength is 0.613 angstrom\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "V=400; #voltage(V)\n", "\n", "#Calculation\n", "lamda=12.26/math.sqrt(V); #de broglie wavelength(angstrom)\n", "\n", "#Result\n", "print \"de broglie wavelength is\",lamda,\"angstrom\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.3, Page number 6.8" ] }, { "cell_type": "code", "execution_count": 10, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "de broglie wavelength is 0.181 nm\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "m=1.674*10**-27; #mass of proton(kg)\n", "h=6.626*10**-34; #planck's constant\n", "E=0.025*1.6*10**-19; #energy(J)\n", "\n", "#Calculation\n", "lamda=h/math.sqrt(2*m*E); #de broglie wavelength(m)\n", "\n", "#Result\n", "print \"de broglie wavelength is\",round(lamda*10**9,3),\"nm\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.4, Page number 6.9" ] }, { "cell_type": "code", "execution_count": 12, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "de broglie wavelength is 0.3065 angstrom\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "V=1600; #voltage(V)\n", "\n", "#Calculation\n", "lamda=12.26/math.sqrt(V); #de broglie wavelength(angstrom)\n", "\n", "#Result\n", "print \"de broglie wavelength is\",lamda,\"angstrom\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.5, Page number 6.14" ] }, { "cell_type": "code", "execution_count": 1, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "uncertainity in momentum is 5.27 *10**-24 kg m/s\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "deltax=0.2*10**-10; #distance(m)\n", "h=6.626*10**-34; #planck's constant\n", "\n", "#Calculation\n", "deltap=h/(2*math.pi*deltax); #uncertainity in momentum(kg m/s)\n", "\n", "#Result\n", "print \"uncertainity in momentum is\",round(deltap*10**24,2),\"*10**-24 kg m/s\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.6, Page number 6.21" ] }, { "cell_type": "code", "execution_count": 7, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "lowest energy of electron is 112.9 eV\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "n1=n2=n3=1;\n", "h=6.62*10**-34; #planck's constant\n", "m=9.1*10**-31; #mass(kg)\n", "L=0.1*10**-9; #side(m) \n", "\n", "#Calculation\n", "E1=h**2*(n1**2+n2**2+n3**2)/(8*m*1.6*10**-19*L**2); #lowest energy of electron(eV)\n", "\n", "#Result\n", "print \"lowest energy of electron is\",round(E1,1),\"eV\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.7, Page number 6.22" ] }, { "cell_type": "code", "execution_count": 9, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "lowest energy of electron is 1.208 *10**4 eV\n", "value of E112, E121, E211 is 2.4168 *10**4 eV\n", "value of E122, E212, E221 is 3.625 *10**4 eV\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "n1=n2=n3=1;\n", "h=6.62*10**-34; #planck's constant\n", "m=8.5*10**-31; #mass(kg)\n", "L=10**-11; #side(m) \n", "\n", "#Calculation\n", "E111=h**2*(n1**2+n2**2+n3**2)/(8*m*1.6*10**-19*L**2); #lowest energy of electron(eV)\n", "E112=6*h**2/(8*m*1.6*10**-19*L**2); #value of E112(eV)\n", "E121=E112; #value of E121(eV)\n", "E211=E112; #value of E211(eV)\n", "E122=9*h**2/(8*m*1.6*10**-19*L**2); #value of E122(eV)\n", "E212=E122; #value of E212(eV)\n", "E221=E122; #value of E221(eV)\n", "\n", "#Result\n", "print \"lowest energy of electron is\",round(E111/10**4,3),\"*10**4 eV\"\n", "print \"value of E112, E121, E211 is\",round(E121/10**4,4),\"*10**4 eV\"\n", "print \"value of E122, E212, E221 is\",round(E122/10**4,3),\"*10**4 eV\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.8, Page number 6.23" ] }, { "cell_type": "code", "execution_count": 12, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "de broglie wavelength is 0.0275 nm\n" ] } ], "source": [ "#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", "h=6.626*10**-34; #planck's constant\n", "E=2000*1.6*10**-19; #energy(J)\n", "\n", "#Calculation\n", "lamda=h/math.sqrt(2*m*E); #de broglie wavelength(m)\n", "\n", "#Result\n", "print \"de broglie wavelength is\",round(lamda*10**9,4),\"nm\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.9, Page number 6.23" ] }, { "cell_type": "code", "execution_count": 15, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "lowest energy of electron is 0.377 *10**-18 joule\n", "answer varies due to rounding off errors\n" ] } ], "source": [ "#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", "h=6.626*10**-34; #planck's constant\n", "n=1;\n", "L=4*10**-10; #side(m) \n", "\n", "#Calculation\n", "E1=n**2*h**2/(8*m*L**2); #lowest energy of electron(joule)\n", "\n", "\n", "#Result\n", "print \"lowest energy of electron is\",round(E1*10**18,3),\"*10**-18 joule\"\n", "print \"answer varies due to rounding off errors\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.10, Page number 6.24" ] }, { "cell_type": "code", "execution_count": 17, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "lowest energy of electron is 0.6031 *10**-17 joule\n", "energy of electron in 1st state is 2.412 *10**-17 joule\n", "energy of electron in 2nd state is 5.428 *10**-17 joule\n" ] } ], "source": [ "#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", "h=6.626*10**-34; #planck's constant\n", "n1=1;\n", "n2=2;\n", "n3=3;\n", "L=1*10**-10; #side(m) \n", "\n", "#Calculation\n", "E1=n1**2*h**2/(8*m*L**2); #lowest energy of electron(joule)\n", "E2=n2**2*h**2/(8*m*L**2); #energy of electron in 1st state(joule)\n", "E3=n3**2*h**2/(8*m*L**2); #energy of electron in 2nd state(joule)\n", "\n", "#Result\n", "print \"lowest energy of electron is\",round(E1*10**17,4),\"*10**-17 joule\"\n", "print \"energy of electron in 1st state is\",round(E2*10**17,3),\"*10**-17 joule\"\n", "print \"energy of electron in 2nd state is\",round(E3*10**17,3),\"*10**-17 joule\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.11, Page number 6.25" ] }, { "cell_type": "code", "execution_count": 24, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "velocity is 4386 km/s\n", "kinetic energy is 54.71 eV\n" ] } ], "source": [ "#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", "h=6.626*10**-34; #planck's constant\n", "lamda=1.66*10**-10; #wavelength(m)\n", "\n", "#Calculation\n", "v=h/(m*lamda); #velocity(m/s)\n", "KE=(1/2)*m*v**2; #kinetic energy(eV)\n", "\n", "#Result\n", "print \"velocity is\",int(v/10**3),\"km/s\"\n", "print \"kinetic energy is\",round(KE/(1.6*10**-19),2),\"eV\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.12, Page number 6.25" ] }, { "cell_type": "code", "execution_count": 27, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "de broglie wavelength is 0.1 angstrom\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "V=15000; #voltage(V)\n", "\n", "#Calculation\n", "lamda=12.26/math.sqrt(V); #de broglie wavelength(angstrom)\n", "\n", "#Result\n", "print \"de broglie wavelength is\",round(lamda,1),\"angstrom\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.13, Page number 6.26" ] }, { "cell_type": "code", "execution_count": 33, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "spacing of crystal is 0.3816 angstrom\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "V=344; #voltage(V)\n", "n=1;\n", "theta=60*math.pi/180; #angle(radian)\n", "\n", "#Calculation\n", "lamda=round(12.26/math.sqrt(V),3); #de broglie wavelength(angstrom)\n", "d=n*lamda/(2*math.sin(theta)); #spacing of crystal(angstrom)\n", "\n", "#Result\n", "print \"spacing of crystal is\",round(d,4),\"angstrom\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 6.14, Page number 6.26" ] }, { "cell_type": "code", "execution_count": 36, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "wavelength is 9.787 *10**-6 m\n", "answer varies due to rounding off errors\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "E=1.5*9.1*10**-31; #energy(joule)\n", "m=1.676*10**-27; #mass(kg)\n", "h=6.62*10**-34; #planck's constant\n", "\n", "#Calculation\n", "v=math.sqrt(2*E/m); \n", "lamda=h/(m*v); #wavelength(m)\n", "\n", "#Result\n", "print \"wavelength is\",round(lamda*10**6,3),\"*10**-6 m\"\n", "print \"answer varies due to rounding off errors\"" ] } ], "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": "2.7.9" } }, "nbformat": 4, "nbformat_minor": 0 }