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diff --git a/Solid_State_Physics_by_Dr._M._Arumugam/Chapter8_D7glvQg.ipynb b/Solid_State_Physics_by_Dr._M._Arumugam/Chapter8_D7glvQg.ipynb new file mode 100644 index 00000000..8d27e900 --- /dev/null +++ b/Solid_State_Physics_by_Dr._M._Arumugam/Chapter8_D7glvQg.ipynb @@ -0,0 +1,280 @@ +{ + "cells": [ + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "# 8: Semiconductor Physics" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example number 1, Page number 8.19" + ] + }, + { + "cell_type": "code", + "execution_count": 1, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "number of electron hole pairs is 2.32 *10**16 per cubic metre\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", + "ni1=2.5*10**19; #number of electron hole pairs\n", + "T1=300; #temperature(K)\n", + "Eg1=0.72*1.6*10**-19; #energy gap(J)\n", + "k=1.38*10**-23; #boltzmann constant\n", + "T2=310; #temperature(K)\n", + "Eg2=1.12*1.6*10**-19; #energy gap(J)\n", + "\n", + "#Calculation\n", + "x1=-Eg1/(2*k*T1);\n", + "y1=(T1**(3/2))*math.exp(x1);\n", + "x2=-Eg2/(2*k*T2);\n", + "y2=(T2**(3/2))*math.exp(x2);\n", + "ni=ni1*(y2/y1); #number of electron hole pairs\n", + "\n", + "#Result\n", + "print \"number of electron hole pairs is\",round(ni/10**16,2),\"*10**16 per cubic metre\"\n", + "print \"answer varies due to rounding off errors\"" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example number 2, Page number 8.20" + ] + }, + { + "cell_type": "code", + "execution_count": 13, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "intrinsic conductivity is 2.016 ohm-1 metre-1\n", + "intrinsic resistivity is 0.496 ohm metre\n", + "number of germanium atoms per m**3 is 4.5 *10**28\n", + "new value of conductivity is 1.434 *10**4 ohm-1 metre-1\n", + "new value of resistivity is 0.697 *10**-4 ohm metre\n", + "answer for new values given in the book varies due to rounding off errors\n" + ] + } + ], + "source": [ + "#importing modules\n", + "import math\n", + "from __future__ import division\n", + "\n", + "#Variable declaration\n", + "w=72.6; #atomic weight\n", + "d=5400; #density(kg/m**3)\n", + "Na=6.025*10**26; #avagadro number\n", + "mew_e=0.4; #mobility of electron(m**2/Vs)\n", + "mew_h=0.2; #mobility of holes(m**2/Vs)\n", + "e=1.6*10**-19;\n", + "m=9.108*10**-31; #mass(kg)\n", + "ni=2.1*10**19; #number of electron hole pairs\n", + "Eg=0.7; #band gap(eV)\n", + "k=1.38*10**-23; #boltzmann constant\n", + "h=6.625*10**-34; #plancks constant\n", + "T=300; #temperature(K)\n", + "\n", + "#Calculation\n", + "sigma=ni*e*(mew_e+mew_h); #intrinsic conductivity(ohm-1 m-1)\n", + "rho=1/sigma; #resistivity(ohm m)\n", + "n=Na*d/w; #number of germanium atoms per m**3\n", + "p=n/10**5; #boron density\n", + "sigman=p*e*mew_h; #new value of conductivity(ohm-1 metre-1)\n", + "rhon=1/sigman; #new value of resistivity(ohm metre)\n", + "\n", + "#Result\n", + "print \"intrinsic conductivity is\",sigma,\"ohm-1 metre-1\"\n", + "print \"intrinsic resistivity is\",round(rho,3),\"ohm metre\"\n", + "print \"number of germanium atoms per m**3 is\",round(n/10**28,1),\"*10**28\"\n", + "print \"new value of conductivity is\",round(sigman/10**4,3),\"*10**4 ohm-1 metre-1\"\n", + "print \"new value of resistivity is\",round(rhon*10**4,3),\"*10**-4 ohm metre\"\n", + "print \"answer for new values given in the book varies due to rounding off errors\"" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example number 3, Page number 8.21" + ] + }, + { + "cell_type": "code", + "execution_count": 14, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "charge carrier density is 2 *10**22 per m**3\n", + "electron mobility is 0.035 m**2/Vs\n" + ] + } + ], + "source": [ + "#importing modules\n", + "import math\n", + "from __future__ import division\n", + "\n", + "#Variable declaration\n", + "e=1.6*10**-19;\n", + "RH=3.66*10**-4; #hall coefficient(m**3/coulomb)\n", + "sigma=112; #conductivity(ohm-1 m-1)\n", + "\n", + "#Calculation\n", + "ne=3*math.pi/(8*RH*e); #charge carrier density(per m**3)\n", + "mew_e=sigma/(e*ne); #electron mobility(m**2/Vs)\n", + "\n", + "#Result\n", + "print \"charge carrier density is\",int(ne/10**22),\"*10**22 per m**3\"\n", + "print \"electron mobility is\",round(mew_e,3),\"m**2/Vs\"" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example number 4, Page number 8.21" + ] + }, + { + "cell_type": "code", + "execution_count": 16, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "intrinsic conductivity is 0.432 *10**-3 ohm-1 m-1\n", + "conductivity during donor impurity is 10.4 ohm-1 m-1\n", + "conductivity during acceptor impurity is 4 ohm-1 m-1\n" + ] + } + ], + "source": [ + "#importing modules\n", + "import math\n", + "from __future__ import division\n", + "\n", + "#Variable declaration\n", + "mew_e=0.13; #mobility of electron(m**2/Vs)\n", + "mew_h=0.05; #mobility of holes(m**2/Vs)\n", + "e=1.6*10**-19;\n", + "ni=1.5*10**16; #number of electron hole pairs\n", + "N=5*10**28;\n", + "\n", + "#Calculation\n", + "sigma1=ni*e*(mew_e+mew_h); #intrinsic conductivity(ohm-1 m-1)\n", + "ND=N/10**8;\n", + "n=ni**2/ND;\n", + "sigma2=ND*e*mew_e; #conductivity(ohm-1 m-1)\n", + "sigma3=ND*e*mew_h; #conductivity(ohm-1 m-1)\n", + "\n", + "#Result\n", + "print \"intrinsic conductivity is\",round(sigma1*10**3,3),\"*10**-3 ohm-1 m-1\"\n", + "print \"conductivity during donor impurity is\",sigma2,\"ohm-1 m-1\"\n", + "print \"conductivity during acceptor impurity is\",int(sigma3),\"ohm-1 m-1\"" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example number 5, Page number 8.22" + ] + }, + { + "cell_type": "code", + "execution_count": 18, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "conductivity is 4.97 mho m-1\n" + ] + } + ], + "source": [ + "#importing modules\n", + "import math\n", + "from __future__ import division\n", + "\n", + "#Variable declaration\n", + "e=1.6*10**-19;\n", + "Eg=0.72; #band gap(eV)\n", + "k=1.38*10**-23; #boltzmann constant\n", + "T1=293; #temperature(K)\n", + "T2=313; #temperature(K)\n", + "sigma1=2; #conductivity(mho m-1)\n", + "\n", + "#Calculation\n", + "x=(Eg*e/(2*k))*((1/T1)-(1/T2));\n", + "y=round(x/2.303,3);\n", + "z=round(math.log10(sigma1),3);\n", + "log_sigma2=y+z;\n", + "sigma2=10**log_sigma2; #conductivity(mho m-1)\n", + "\n", + "#Result\n", + "print \"conductivity is\",round(sigma2,2),\"mho m-1\"" + ] + } + ], + "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 +} |