{ "cells": [ { "cell_type": "markdown", "metadata": {}, "source": [ "#4: Electron Theory of Metals" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 4.1, Page number 4.28" ] }, { "cell_type": "code", "execution_count": 12, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "energy difference is 1.81 *10**-37 J\n", "3/2*k*T = E2 = 3.62 *10**-37 J\n", "T = 1.75 *10**-14 K\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", "nx=ny=nz=1;\n", "n=6;\n", "a=1; #edge(m)\n", "h=6.63*10**-34; #planck's constant\n", "k=1.38\n", "#Calculation\n", "E1=h**2*(nx**2+ny**2+nz**2)/(8*m*a**2);\n", "E2=h**2*n/(8*m*a**2);\n", "E=E2-E1; #energy difference(J)\n", "T=(2*E2*10**37)/(3*k*10**-23)\n", "#Result\n", "print \"energy difference is\",round(E*10**37,2),\"*10**-37 J\"\n", "print \"3/2*k*T = E2 =\",round(E2*10**37,2),\"*10**-37 J\"\n", "print \"T =\",round(T/10**23,2),\"*10**-14 K\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 4.2, Page number 4.28" ] }, { "cell_type": "code", "execution_count": 13, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "temperature is 1261 K\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", "y=1/100; #percentage of probability\n", "x=0.5*1.6*10**-19; #energy(J)\n", "k=1.38*10**-23; #boltzmann constant\n", "\n", "#Calculation\n", "xbykT=math.log((1/y)-1);\n", "T=x/(k*xbykT); #temperature(K)\n", "\n", "#Result\n", "print \"temperature is\",int(T),\"K\"\n", "print \"answer varies due to rounding off errors\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 4.3, Page number 4.29" ] }, { "cell_type": "code", "execution_count": 4, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "fermi energy is 3.2 eV\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "d=970; #density(kg/m**3)\n", "Na=6.02*10**26; #avagadro number\n", "w=23; #atomic weight\n", "m=9.1*10**-31; #mass(kg)\n", "h=6.62*10**-34; #planck's constant\n", "\n", "#Calculation\n", "N=d*Na/w; #number of atoms/m**3\n", "x=h**2/(8*m);\n", "y=(3*N/math.pi)**(2/3);\n", "EF=x*y; #fermi energy(J)\n", "\n", "#Result\n", "print \"fermi energy is\",round(EF/(1.6*10**-19),1),\"eV\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 4.4, Page number 4.29" ] }, { "cell_type": "code", "execution_count": 3, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "p(E) = 0.269\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "kT=1;\n", "E_EF=1;\n", "\n", "#Calculations\n", "p_E=1/(1+math.exp(E_EF/kT)) \n", " \n", "#Result \n", "print \"p(E) =\",round(p_E,3)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 4.5, Page number 4.29" ] }, { "cell_type": "code", "execution_count": 28, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "N = 2.4 *10**26 states\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "from scipy.integrate import quad \n", "\n", "#Variable declarations\n", "m=9.1*10**-31\n", "h=6.626*10**-34\n", "Ef=3.1\n", "Ef1=Ef+0.02\n", "e=1.6*10**-19\n", "#Calculations\n", "def zintg(E):\n", " return math.pi*((8*m)**(3/2))*(E**(1/2)*e**(3/2))/(2*(h**3))\n", "N=quad(zintg,Ef,Ef1)[0]\n", "\n", "#Result\n", "print\"N =\",round(N*10**-26,1),\"*10**26 states\"" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 4.6, Page number 4.30" ] }, { "cell_type": "code", "execution_count": 1, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "n = 8.5 *10**28 /m**3\n", "The drift speed Vd = 36.6 *10**-5 m/s\n", "The mean free collision time Tc = 2.087 *10**-14 seconds\n", "Mean free path = 3.34 *10**-8 m(answer varies due to rounding off errors)\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "N=6.023*10**26 #Avagadro number\n", "D=8960 #density \n", "F_e=1 #no.of free electrons per atom \n", "W=63.54 #Atomic weight\n", "i=10\n", "e=1.602*10**-19\n", "m=9.1*10**-31\n", "rho=2*10**-8\n", "Cbar=1.6*10**6 #mean thermal velocity(m/s)\n", "\n", "#Calculations\n", "n=(N*D*F_e)/W\n", "A=math.pi*0.08**2*10**-4\n", "Vd=i/(A*n*e) #Drift speed\n", "Tc=m/(n*(e**2)*rho)\n", "lamda=Tc*Cbar\n", "\n", "#Result\n", "print\"n =\",round(n/10**28,1),\"*10**28 /m**3\"\n", "print\"The drift speed Vd =\",round(Vd*10**5,1),\"*10**-5 m/s\"\n", "print\"The mean free collision time Tc =\",round(Tc*10**14,3),\"*10**-14 seconds\"\n", "print\"Mean free path =\",round(lamda*10**8,2),\"*10**-8 m\"\"(answer varies due to rounding off errors)\" \n", "\n" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 4.7, Page number 4.30" ] }, { "cell_type": "code", "execution_count": 5, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "The mean free collision time = 4.8 *10**7 ohm**-1 m**-1\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "##Variable declaration\n", "n=8.5*10**28\n", "e=1.602*10**-19\n", "t=2*10**-14\n", "m=9.1*10**-31\n", "\n", "#Calculations\n", "Tc=n*(e**2)*t/m\n", "\n", "#Result\n", "print \"The mean free collision time =\",round(Tc/10**7,1),\"*10**7 ohm**-1 m**-1\"\n" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 4.8, Page number 4.31" ] }, { "cell_type": "code", "execution_count": 12, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "Relaxation time = 4.0 *10**-14 second\n", "Mobility = 7.0 *10**-3 m**2/volt-s\n", "Drift Velocity= 0.7 m/s\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "\n", "#Variable declaration\n", "e=1.6*10**-19\n", "E=1 #(V/m)\n", "rho=1.54*10**-8\n", "n=5.8*10**28\n", "\n", "#Calculations\n", "T=m/(rho*n*e**2)\n", "Me=(e*T)/m\n", "Vd=Me*E\n", "\n", "#Result \n", "print\"Relaxation time =\",round(T*10**14),\"*10**-14 second\"\n", "print\"Mobility =\",round(Me*10**3),\"*10**-3 m**2/volt-s\"\n", "print\"Drift Velocity=\",round(Vd*100,1),\"m/s\"\n" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 4.9, Page number 4.31" ] }, { "cell_type": "code", "execution_count": 9, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "Temperature coefficient of resistivity,a = 5.7\n", "rho_973 = 5.51 *10**-8 ohm-m\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "\n", "##Variable declaration\n", "rho_r=0\n", "T=300\n", "rho=1.7*10**-18\n", "\n", "#Calculations \n", "a=rho/T\n", "rho_973=a*973\n", "\n", "#Results\n", "print\"Temperature coefficient of resistivity,a =\",round(a*10**21,1)\n", "print\"rho_973 =\",round(rho_973*10**18,2),\"*10**-8 ohm-m\"\n" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "##Example number 4.10, Page number 4.31" ] }, { "cell_type": "code", "execution_count": 10, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "Increase in resistivity in copper = 0.54 *10**-8 ohm m\n", "Total resistivity of copper alloy = 2.04 *10**-8 ohm m\n", "The resistivity of alloy at 3K = 0.54 *10**-8 ohm m\n" ] } ], "source": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "\n", "##Variable declaration\n", "rho1=1.2*10**-8\n", "p1=0.4\n", "rho2=0.12*10**-8\n", "p2=0.5\n", "rho3=1.5*10**-8\n", "#Calculations\n", "R=(rho1*p1)+(rho2*p2)\n", "R_c=R+rho3\n", "\n", "#Results\n", "print\"Increase in resistivity in copper =\",round(R*10**8,2),\"*10**-8 ohm m\"\n", "print\"Total resistivity of copper alloy =\",round(R_c*10**8,2),\"*10**-8 ohm m\"\n", "print\"The resistivity of alloy at 3K =\",round(R*10**8,2),\"*10**-8 ohm m\"" ] } ], "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 }