{ "metadata": { "name": "", "signature": "sha256:d42b95d086e994736fd89da8bf44c85325c991b363e30dcf52a4839620130b97" }, "nbformat": 3, "nbformat_minor": 0, "worksheets": [ { "cells": [ { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "Ch-3 Electroluminescent Sources" ] }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 3.1 Page no 80" ] }, { "cell_type": "code", "collapsed": false, "input": [ "from __future__ import division\n", "from math import log\n", "#Calculation of barrier potential\n", "#Given data\n", "p=5# # Resistivity of p-region\n", "n=2# # Resistivity of n-region\n", "mu=3900#\n", "k=0.026# #Boltzmann constant\n", "ni=2.5*10**13# #Density of the electron hole pair\n", "e=1.6*10**-19# #charge of electron\n", " \n", "#Barrier potential calculation\n", "r0=(1/p)# # Reflection at the fiber air interface \n", "r1=(1/n)#\n", "m=r1/(mu*e)#\n", "p=6.5*10**14# #Density of hole in p -region\n", "Vb=k*log(p*m/ni**2)#\n", "print \"Barrier potential = %0.3f V\"%Vb\n", "\n", "# The answers vary due to round off error" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Barrier potential = 0.175 V\n" ] } ], "prompt_number": 19 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 3.15 Page no 484" ] }, { "cell_type": "code", "collapsed": false, "input": [ "# Calculation of external efficiency \n", "#Given data\n", "ne1=0.20# #Total efficiency \n", "V=3# # Voltage applied\n", "Eg=1.43# # Bandgap energy\n", "\n", "# External efficiency\n", "ne=(ne1*Eg/V)*100#\n", "print \"External efficiency of the device = %0.1f %% \"%(ne)#" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "External efficiency of the device = 9.5 % \n" ] } ], "prompt_number": 6 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 3.16 Page no 484" ] }, { "cell_type": "code", "collapsed": false, "input": [ "from math import exp\n", "# Calculation of ratio of threshold current densities\n", "# Given data\n", "To1=160# # Device temperature\n", "To2=55# # Device temperature\n", "T1=293#\n", "T2=353#\n", "J81=exp(T1/To1)# # Threshold current density \n", "J21=exp(T2/To1)#\n", "J82=exp(T1/To2)## \n", "J22=exp(T2/To2)## \n", "cd1=J21/J81# # Ratio of threshold current densities\n", "cd2=J22/J82#\n", "\n", "print\"Ratio of threshold current densities= %0.2f \"%(cd1)\n", "print\"Ratio of threshold current densities= %0.2f \"%(cd2)" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Ratio of threshold current densities= 1.45 \n", "Ratio of threshold current densities= 2.98 \n" ] } ], "prompt_number": 9 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 3.17 Page no 484" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#Computation of conversion efficiency \n", "#Given data\n", "i=10*10**-6# # Device current\n", "p=5# # Electrical power\n", "op=50 *10**-6# # Optical power\n", "ip=5*10*10**-3# # Input power\n", "\n", "#Conversion efficiency\n", "c=op/ip*100# \n", "print \"Conversion efficiency = %0.1f %% \"%(c)" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Conversion efficiency = 0.1 % \n" ] } ], "prompt_number": 18 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 3.18 Page no 485" ] }, { "cell_type": "code", "collapsed": false, "input": [ "# Calculation of total power emitted\n", "#Given data\n", "r=0.7# # Emissivity\n", "r0=5.67*10**-8# # Stephen's constant\n", "A=10**-4# # Surface area\n", "T=2000# # Temperature\n", "\n", "# Total power emitted\n", "P=r*r0*A*T**4# \n", "\n", "print\"Total power emitted = %0.1f Watts \"%P" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Total power emitted = 63.5 Watts \n" ] } ], "prompt_number": 14 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 3.19 Page no 485" ] }, { "cell_type": "code", "collapsed": false, "input": [ "# Computation of total energy\n", "#Given data\n", "h=6.63*10**-34# # Planck constant\n", "v=5*10**14# # Bandgap frequency of laser\n", "N=10**24# # Population inversion density\n", "V=10**-5# # Volume of laser medium\n", "\n", "# Total energy\n", "E=(1/2)*h*v*(N)*V# \n", "\n", "print \"Total energy = %0.1f J \"%E" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Total energy = 1.7 J \n" ] } ], "prompt_number": 13 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 3.20 Page no 485" ] }, { "cell_type": "code", "collapsed": false, "input": [ "# Computation of pulse power\n", "# Given data\n", "L=0.1# # Length of laser\n", "R=0.8# # Mirror reflectance of end mirror\n", "E=1.7# # Laser pulse energy\n", "c=3*10**8# # Velocity of light\n", "t=L/((1-R)*c)# # Cavity life time\n", "\n", "# Pulse power\n", "p=E/t# \n", "\n", "print\"Pulse power = %0.0f W \"%p" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Pulse power = 1020000000 W \n" ] } ], "prompt_number": 20 } ], "metadata": {} } ] }