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author | hardythe1 | 2015-06-17 11:14:34 +0530 |
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committer | hardythe1 | 2015-06-17 11:14:34 +0530 |
commit | 37d315828bbfc0f5cabee669d2b9dd8cd17b5154 (patch) | |
tree | 18b9d2929b329e112462bca900e9ae25c4c03006 /Engineering_Physics_By_G_Vijayakumari/Chapter9.ipynb | |
parent | 79c59acc7af08ede23167b8455de4b716f77601f (diff) | |
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diff --git a/Engineering_Physics_By_G_Vijayakumari/Chapter9.ipynb b/Engineering_Physics_By_G_Vijayakumari/Chapter9.ipynb new file mode 100755 index 00000000..90c89eeb --- /dev/null +++ b/Engineering_Physics_By_G_Vijayakumari/Chapter9.ipynb @@ -0,0 +1,585 @@ +{
+ "cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "#9: Energy bands in solids"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.1, Page number 240"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 29,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The fermi function for an energy kt above fermi energy is 0.269\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "#E-EF=KT\n",
+ "#K=KB is the boltzmann constant in m^2 Kg s^-2 k^-1\n",
+ "\n",
+ "#Calculation\n",
+ "f=1/(1+math.exp(1)); #The fermi function for an energy kt above fermi energy\n",
+ "\n",
+ "#Result\n",
+ "print \"The fermi function for an energy kt above fermi energy is\",round(f,3)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.2, Page number 240"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 32,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The fermi function is 0.358999\n",
+ "answer given in the book is wrong\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "X=0.01*1.6*10**-19; #difference between energy and fermi energy(J)\n",
+ "T=200; #temperature(K)\n",
+ "KB=1.38*10**-23; #Boltzmann's Constant(J/K)\n",
+ "\n",
+ "#Calculation\n",
+ "f=1/(1+math.exp(X/(KB*T))); #The fermi function\n",
+ "\n",
+ "#Result\n",
+ "print \"The fermi function is\",round(f,6)\n",
+ "print \"answer given in the book is wrong\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.3, Page number 241"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 37,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The fermi velocity fo conducting electron in aluminium is 2.02118 *10**6 ms^-1\n",
+ "The mean free path for conducting electron of aluminium is 14.7546 nm\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "EF=11.63*1.6*10**-19; #fermi energy of conducting electron in aluminium(J)\n",
+ "t=7.3*10**-15; #relaxation time for electron(sec)\n",
+ "m=9.11*10**-31; #mass of electon(Kg)\n",
+ "\n",
+ "#Calculation\n",
+ "Vf=math.sqrt(2*EF/m); #The fermi velocity fo conducting electron in aluminium(ms^-1)\n",
+ "x=t*Vf*10**9; #mean free path for conducting electron of aluminium(nm)\n",
+ "\n",
+ "#Result\n",
+ "print \"The fermi velocity fo conducting electron in aluminium is\",round(Vf/10**6,5),\"*10**6 ms^-1\"\n",
+ "print \"The mean free path for conducting electron of aluminium is\",round(x,4),\"nm\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.4, Page number 241"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 46,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The fermi energy in a metal is 3.36888 *10**-19 J or 2.1055 eV\n",
+ "The fermi temperature in a metal is 24.41 *10**3 K\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "Vf=0.86*10**6; #The femi energy of electons in the metal(m/sec)\n",
+ "m=9.11*10**-31; #mass of electon(Kg)\n",
+ "KB=1.38*10**-23; #Boltzmann's Constant(m^2 Kg s^-2 k^-1)\n",
+ "\n",
+ "#Calculation\n",
+ "Ef=(1/2)*m*Vf**2; #The fermi energy in a metal(J)\n",
+ "Tf=Ef/KB; #The fermi temperature in a metal(K)\n",
+ "\n",
+ "#Result\n",
+ "print \"The fermi energy in a metal is\",round(Ef/10**-19,5),\"*10**-19 J or\",round(Ef/(1.6*10**-19),4),\"eV\"\n",
+ "print \"The fermi temperature in a metal is\",round(Tf/10**3,2),\"*10**3 K\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.5, Page number 242"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 3,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The fermi temparature for sodium is 37.1 *10**3 K\n",
+ "The fermi velocity fo conducting electron in aluminium is 1.0602 *10**6 ms^-1\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "Ef=3.2*1.6*10**-19; #The fermi energy in a metal(J)\n",
+ "m=9.11*10**-31; #mass of electon(Kg)\n",
+ "KB=1.38*10**-23; #Boltzmann's Constant(m^2 Kg s^-2 k^-1)\n",
+ "\n",
+ "#Calculation\n",
+ "Tf=Ef/KB; #The fermi temparature for sodium(K)\n",
+ "Vf=math.sqrt(2*Ef/m); #The fermi velocity fo conducting electron in aluminium(ms^-1)\n",
+ "\n",
+ "#Result\n",
+ "print \"The fermi temparature for sodium is\",round(Tf/10**3,2),\"*10**3 K\"\n",
+ "print \"The fermi velocity fo conducting electron in aluminium is\",round(Vf/10**6,4),\"*10**6 ms^-1\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.6, Page number 242"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 7,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The temperature at which there is 1% probability that an electron in a solid is 1.26158 *10**3 K\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "E=5.5*1.6*10**-19; #energy level(J)\n",
+ "Ef=5*1.6*10**-19; #fermi energy level(J)\n",
+ "x=0.5*1.6*10**-19; #Difference between energy and fermi energy(J)\n",
+ "f=0.01; #fermi function at which there is 1% probability that an electron in a solid\n",
+ "KB=1.38*10**-23; #Boltzmann's Constant(m^2 Kg s^-2 k^-1)\n",
+ "\n",
+ "#Calculation\n",
+ "T=x/(KB*(math.log(1-f)-math.log(f))); #The temperature at which there is 1% probability that an electron in a solid(K)\n",
+ "\n",
+ "#Result\n",
+ "print \"The temperature at which there is 1% probability that an electron in a solid is\",round(T/10**3,5),\"*10**3 K\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.7, Page number 244"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 9,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The energy for probability of occupancy at 1st is 1.98 eV\n",
+ "The energy for probability of occupancy at 2nd is 2.219 eV\n",
+ "The energy for probability of occupancy at 3rd is 2.1 eV\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "Ef=2.1*1.6*10**-19; #fermi energy level in potassium(J)\n",
+ "f1=0.99; #fermi factor for 1st\n",
+ "f2=0.01; #fermi factor for 2nd\n",
+ "f3=0.5; #fermi factor for 3rd\n",
+ "T=300; #temperature(K)\n",
+ "e=1.6*10**-19; #charge of electron(C)\n",
+ "KB=1.38*10**-23; #Boltzmann's Constant(m^2 Kg s^-2 k^-1)\n",
+ "\n",
+ "#Calculation\n",
+ "E1=(Ef+((KB*T)*(math.log(1-f1)-math.log(f1))))/e; #The energy for probability of occupancy at 1st(eV)\n",
+ "E2=(Ef+((KB*T)*(math.log(1-f2)-math.log(f2))))/e; #The energy for 1st at which the probability of occupancy(eV)\n",
+ "E3=(Ef+((KB*T)*(math.log(1-f3)-math.log(f3))))/e; #The energy for 1st at which the probability of occupancy(eV)\n",
+ "\n",
+ "#Result\n",
+ "print \"The energy for probability of occupancy at 1st is\",round(E1,2),\"eV\"\n",
+ "print \"The energy for probability of occupancy at 2nd is\",round(E2,3),\"eV\"\n",
+ "print \"The energy for probability of occupancy at 3rd is\",E3,\"eV\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.8, Page number 245"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 11,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The probability of unoccupancy by an electron at room temperature is 0.97946\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "X=0.1*1.6*10**-19; #difference between energy and fermi energy(J)\n",
+ "T=300; #temperature(K)\n",
+ "KB=1.38*10**-23; #Boltzmann's Constant(m^2 Kg s^-2 k^-1)\n",
+ "\n",
+ "#Calculation\n",
+ "f=1-1/(1+math.exp(X/(KB*T))); #The probability of unoccupancy by an electron at room temperature \n",
+ "\n",
+ "#Result\n",
+ "print \"The probability of unoccupancy by an electron at room temperature is\",round(f,5)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.9, Page number 252"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 18,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The fermi energy for the metal is 11.66 eV\n",
+ "The fermi factor is 0.0205\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "n=4; #number of atoms/unit cell in Al\n",
+ "a=4.05*10**-10; #lattice constant of Aluminium which is FCC crystal(m)\n",
+ "nf=3; #number of free electrons per atom in Al\n",
+ "T=300; #ambient temperature(K)\n",
+ "x=0.1*1.6*10**-19; #The same difference energy and fermi energy(J)\n",
+ "m=9.11*10**-31; #mass of electon(kg)\n",
+ "h=6.625*10**-34; #plank's constant(m^2 Kg/sec)\n",
+ "KB=1.38*10**-23; #Boltzmann's Constant(m^2 Kg s^-2 k^-1)\n",
+ "\n",
+ "#Calculation\n",
+ "nc=n*nf/(a**3); #number of electrons per unit volume\n",
+ "Ef=h**2/(8*m)*((3*nc)/math.pi)**(2/3); #The fermi energy for the metal(eV)\n",
+ "f=1/(1+math.exp(x/(KB*T))); #he fermi factor\n",
+ "\n",
+ "#Result\n",
+ "print \"The fermi energy for the metal is\",round(Ef/(1.6*10**-19),2),\"eV\"\n",
+ "print \"The fermi factor is\",round(f,4)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.10, Page number 253"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 20,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The fermi energy for cesium is 1.537 eV\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "n=2; #number of atoms/unit cell in cesium which is Bcc\n",
+ "a=6.14*10**-10; #lattice constant of cesium which is BCC crystal(m)\n",
+ "nf=1; #number of free electrons per atom in cesium\n",
+ "m=9.11*10**-31; #mass of electon(kg)\n",
+ "h=6.625*10**-34; #plank's constant(m^2 Kg/sec)\n",
+ "KB=1.38*10**-23; #Boltzmann's Constant(m^2 Kg s^-2 k^-1)\n",
+ "e=1.6*10**-19; #charge of electron(C)\n",
+ "\n",
+ "#Calculation\n",
+ "nc=n*nf/(a**3); #number of electrons per unit volume\n",
+ "Ef=(h**2/(8*m)*((3*nc)/math.pi)**(2/3))/e; #The fermi energy for the metal(eV)\n",
+ "\n",
+ "#Result\n",
+ "print \"The fermi energy for cesium is\",round(Ef,3),\"eV\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.11, Page number 254"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 22,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The number of free electrons per unit volume in potassium is 1.38 *10**28 electrons/m^3\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "Ef=2.1*1.6*10**-19; #The fermi energy level in potassium at a particular temperature(J)\n",
+ "m=9.11*10**-31; #mass of electron(kg)\n",
+ "h=6.625*10**-34; #plank's constant(m^2 Kg/sec)\n",
+ "\n",
+ "#Calculation\n",
+ "nc=(8*m/(h**2)*Ef)**(3/2)*(math.pi/3); #ThE Number of free electrons per unit volume in potassium(electrons/m^3)\n",
+ "\n",
+ "#Result\n",
+ "print \"The number of free electrons per unit volume in potassium is\",round(nc/10**28,2),\"*10**28 electrons/m^3\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.12, Page number 254"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 24,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The fermi energy for the sodium is 3.155 eV\n"
+ ]
+ }
+ ],
+ "source": [
+ "#importing modules\n",
+ "import math\n",
+ "from __future__ import division\n",
+ "\n",
+ "#Variable declaration\n",
+ "AW=23; #atomic weight of sodium(gm/mole)\n",
+ "d=0.971*10**6; #density of sodium(gm/m^3)\n",
+ "m=9.11*10**-31; #mass of electon(kg)\n",
+ "h=6.625*10**-34; #plank's constant(m^2 Kg/sec)\n",
+ "AV=6.02*10**23; #Avagadro number(mole^-1)\n",
+ "e=1.6*10**-19; #charge of electron(C)\n",
+ "\n",
+ "#Calculation\n",
+ "nc=AV*d/AW; #number of electrons per unit volume\n",
+ "Ef=(h**2/(8*m)*((3*nc)/math.pi)**(2/3))/e; #The fermi energy for the sodium(eV)\n",
+ "\n",
+ "#Result\n",
+ "print \"The fermi energy for the sodium is\",round(Ef,3),\"eV\""
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "##Example number 9.13, Page number 255"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 26,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "The fermi energy for the sodium is 7.046 eV\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",
+ "AW=63.5; #atomic weight of copper(u)\n",
+ "M=63.5*1.66*10**-27; #mass of one copper atom(kg)\n",
+ "d=8.94*10**3; #density of sodium(Kg/m^3)\n",
+ "m=9.11*10**-31; #mass of electon(Kg)\n",
+ "h=6.625*10**-34; #plank's constant(m^2 Kg/sec)\n",
+ "e=1.6*10**-19; #charge of electron(C)\n",
+ "\n",
+ "#Calculation\n",
+ "nc=d/M; #number of electrons per unit volume(electrons/m^3)\n",
+ "Ef=h**2/(8*m)*((3*nc)/math.pi)**(2/3)/e; #The fermi energy for the sodium(eV)\n",
+ "\n",
+ "#Result\n",
+ "print \"The fermi energy for the sodium is\",round(Ef,3),\"eV\"\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
+}
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