{ "metadata": { "name": "", "signature": "sha256:d8c62a33cdb998cb212b402408ceb0e19f54a33922b51cf1b80232d50d8d2341" }, "nbformat": 3, "nbformat_minor": 0, "worksheets": [ { "cells": [ { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "6: Dielectric Properties" ] }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example number 6.1, Page number 6.23" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "C = 2 #capacitance(micro-farad)\n", "V = 1000 #voltage applied(V)\n", "epsilon_r = 100 #permitivity\n", "\n", "#Calculation\n", "C = C*10**-6 #capacitance(farad)\n", "W = (C*V**2)/2 #energy stored in capacitor(J)\n", "C0 = C/epsilon_r #capacitance removing the dielectric\n", "W0 = C0*(V**2)/2 #energy stored without dielectric(J)\n", "E = 1-W0 #energy stored in dielectric(J)\n", "\n", "#Result\n", "print \"energy stored in capacitor is\",W,\"J\"\n", "print \"energy stored in the dielectric is\",E,\"J\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "energy stored in capacitor is 1.0 J\n", "energy stored in the dielectric is 0.99 J\n" ] } ], "prompt_number": 1 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example number 6.2, Page number 6.24" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "epsilon_r = 4.94\n", "n_2 = 2.69 #square of index of refraction\n", "alpha_i = 0 #at optical frequencies\n", "\n", "#Calculation\n", "#(epsilon_r-1)/(epsilon_r+2) = N*(alpha_e+alpha_i)/(3*epsilon0)\n", "X = (epsilon_r-1)/(epsilon_r+2)\n", "#epsilon_r = n**2. therefore (n**2-1)/(n**2+2) = N*alpha_e/(3*epsilon0)\n", "Y = (n_2-1)/(n_2+2)\n", "#N*(alpha_e+alpha_i)/N*alpha_e = X/Y\n", "#let alpha = alpha_i/alpha_e\n", "alphai_e = (X/Y)-1 #ratio between electronic ionic and electronic polarizability\n", "alphai_e = math.ceil(alphai_e*10**4)/10**4 #rounding off to 4 decimals\n", "alphae_i = 1/alphai_e #ratio between electronic and ionic polarizability\n", "alphae_i = math.ceil(alphae_i*10**3)/10**3 #rounding off to 3 decimals\n", "\n", "#Result\n", "print \"ratio between electronic ionic and electronic polarizability is\",alphai_e\n", "print \"ratio between electronic and ionic polarizability is\",alphae_i" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "ratio between electronic ionic and electronic polarizability is 0.5756\n", "ratio between electronic and ionic polarizability is 1.738\n" ] } ], "prompt_number": 3 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example number 6.3, Page number 6.25" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "epsilon_r = 2.56\n", "tan_delta = 0.7*10**-4\n", "f = 1 #frequency(MHz)\n", "A = 8 #area(cm**2)\n", "d = 0.08 #diameter(mm)\n", "epsilon0 = 8.85*10**-12\n", "\n", "#Calculation\n", "A = A*10**-4 #area(m**2)\n", "d = d*10**-3 #diameter(m)\n", "epsilon_rdash = epsilon_r*tan_delta\n", "omega = 2*math.pi*10**6\n", "Rp = d/(omega*epsilon0*epsilon_rdash*A) #parallel loss resistance(ohm)\n", "Rp = Rp*10**-6 #parallel loss resistance(Mega ohm)\n", "Rp = math.ceil(Rp*10**3)/10**3 #rounding off to 3 decimals\n", "Cp = A*epsilon0*epsilon_r/d #capacitance(farad)\n", "\n", "#Result\n", "print \"parallel loss resistance is\",Rp,\"ohm\"\n", "print \"capacitance in Farad is\",Cp,\"Farad\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "parallel loss resistance is 10.036 ohm\n", "capacitance in Farad is 2.2656e-10 Farad\n" ] } ], "prompt_number": 9 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example number 6.4, Page number 6.26" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "N = 3*10**28 #density(atoms/m**3)\n", "alpha_e = 10**-40 #electronic polarizability(Farad-m**2)\n", "epsilon0 = 8.854*10**-12\n", "\n", "#Calculation\n", "epsilon_r = 1+(N*alpha_e/epsilon0) #dielectric constant of material\n", "epsilon_r = math.ceil(epsilon_r*10**3)/10**3 #rounding off to 3 decimals\n", "\n", "#Result\n", "print \"dielectric constant of material is\",epsilon_r " ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "dielectric constant of material is 1.339\n" ] } ], "prompt_number": 10 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example number 6.5, Page number 6.27" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "epsilon0 = 8.854*10**-12\n", "epsilon_r = 1.0000684 #dielectric constant\n", "N = 2.7*10**25 #density(atoms/m**3)\n", "\n", "#Calculation\n", "alpha_e = epsilon0*(epsilon_r-1)/N #electronic polarizability(Fm**2)\n", "\n", "#Result\n", "print \"electronic polarizability is\",round(alpha_e/1e-41,3),\"*10^-41 Fm**2\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "electronic polarizability is 2.243 *10^-41 Fm**2\n" ] } ], "prompt_number": 12 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example number 6.6, Page number 6.27" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "epsilon0 = 8.85*10**-12\n", "V = 100 #potential(V)\n", "A = 100 #area(cm**2)\n", "d = 1 #plate seperation(cm)\n", "\n", "#Calculation\n", "A = A*10**-4 #area(m**2)\n", "d = d*10**-2 #plate seperation(m)\n", "C = epsilon0*A/d #capacitance(farad)\n", "Q = C*V #charge on plates\n", "\n", "#Result\n", "print \"capacitance of capacitor is\",C,\"F\"\n", "print \"charge on plates in coulomb is\",Q,\"coulomb\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "capacitance of capacitor is 8.85e-12 F\n", "charge on plates in coulomb is 8.85e-10 coulomb\n" ] } ], "prompt_number": 13 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example number 6.7, Page number 6.28" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "N = 6.02*10**26 #avagadro number\n", "d = 2050 #density(kg/m**3)\n", "AW = 32 #atomic weight of sulphur\n", "epsilon_r = 3.75 #relative dielectric constant\n", "epsilon0 = 8.55*10**-12\n", "\n", "#Calculation\n", "n = N*d/AW #number of atoms(per m**3)\n", "alpha_e = ((epsilon_r-1)/(epsilon_r+2))*3*epsilon0/n #electronic polarizability(Fm**2) \n", "\n", "#Result\n", "print \"electronic polarizability is\",round(alpha_e/1e-40,3),\"*10^-40 Fm**2\" " ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "electronic polarizability is 3.181 *10^-40 Fm**2\n" ] } ], "prompt_number": 15 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example number 6.8, Page number 6.29" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "Q = 2*10**-10 #charge(coulomb)\n", "d = 4 #plate seperation(mm)\n", "epsilon_r = 3.5 #dielectric constant\n", "A = 650 #area(mm**2)\n", "epsilon0 = 8.85*10**-12\n", "\n", "#Calculation\n", "d = d*10**-3 #plate seperation(m)\n", "A = A*10**-6 #area(m**2)\n", "V = Q*d/(epsilon0*epsilon_r*A) #voltage across capacitors(V)\n", "V = math.ceil(V*10**3)/10**3 #rounding off to 3 decimals\n", "\n", "#Result\n", "print \"resultant voltage across capacitors is\",V,\"V\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "resultant voltage across capacitors is 39.735 V\n" ] } ], "prompt_number": 16 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example number 6.9, Page number 6.30" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#importing modules\n", "import math\n", "from __future__ import division\n", "\n", "#Variable declaration\n", "V = 10 #potential(V)\n", "d = 2*10**-3 #plate seperation(m)\n", "epsilon_r = 6\n", "epsilon0 = 8.85*10**-12\n", "\n", "#Calculation\n", "E = V/d #electric field(V/m)\n", "D = epsilon0*epsilon_r*E #dielectric displacement(C/m**2)\n", "\n", "#Result\n", "print \"dielectric displacement is\",D,\"Cm^-2\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "dielectric displacement is 2.655e-07 Cm^-2\n" ] } ], "prompt_number": 18 } ], "metadata": {} } ] }