{ "cells": [ { "cell_type": "markdown", "metadata": {}, "source": [ "# Chapter2 - Ray propagation in optical fiber" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 2.1 : Page 21" ] }, { "cell_type": "code", "execution_count": 3, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "part (a)\n", "numerical aperture is 0.244\n", "part (b)\n", "angle αm = 14.13 degree\n", "angle Om = 9.37 degree\n", "angle Φc = 80.63 degree\n", "part (c)\n", "pulse broadning per unit length = 6.76e-11 sm**-1\n" ] } ], "source": [ "from math import degrees, asin, sqrt\n", "#NA ,angles and pulse broadning\n", "print \"part (a)\"\n", "n1=1.5##core refrative index\n", "n2=1.48##claddin refractive index\n", "a=100/2##radius in micro meter\n", "na=1##air refrative index\n", "NA=sqrt(n1**2-n2**2)##numerical aperture\n", "print \"numerical aperture is %0.3f\"%NA\n", "print \"part (b)\"\n", "am=(asin(NA))##\n", "tm=asin(NA/n1)##\n", "tc=asin(n2/n1)##\n", "print \"angle αm = %0.2f degree\"%degrees(am)\n", "print \"angle Om = %0.2f degree\"%degrees(tm)\n", "print \"angle Φc = %0.2f degree\"%degrees(tc)\n", "print \"part (c)\"\n", "c=3*10**8##speed of light in m/s\n", "dtl=((n1/n2)*(n1-n2)/c)##pulse broadning per unit length\n", "print \"pulse broadning per unit length = %0.2e sm**-1\"%dtl" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 2.2 : Page 22" ] }, { "cell_type": "code", "execution_count": 5, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "all other rays will suffer reflections between these two extremes of : 0 and 1650.0 m**-1\n" ] } ], "source": [ "from math import tan\n", "#minimum and maximum number of reflections\n", "n1=1.5##core refrative index\n", "n2=1.48##claddin refractive index\n", "a=100/2##radius in micro meter\n", "na=1##air refrative index\n", "NA=sqrt(n1**2-n2**2)##numerical aperture\n", "am=(asin(NA))##\n", "tm=asin(NA/n1)##\n", "tc=asin(n2/n1)##\n", "L=((a*10**-6)/(tan(tm)))##length in meter\n", "x=(1/(2*L))##maximum number of reflections per meter\n", "print \"all other rays will suffer reflections between these two extremes of :\",(0),\" and \",round(x),\" m**-1\"\n", "#answer is wrong in the textbook" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 2.3 : Page 27" ] }, { "cell_type": "code", "execution_count": 6, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "pulse broadning = 2.45 ns km**-1\n" ] } ], "source": [ "#pulse broadning\n", "h=0.85##WAVELENGTH IN MICRO METER\n", "y=0.035##spectral width\n", "c=0.021##constant\n", "cl=3##speed of light in m/s\n", "dtl=(y/cl)*c##\n", "print \"pulse broadning = %0.2f ns km**-1\"%(dtl*10**4)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 2.4 : Page 27" ] }, { "cell_type": "code", "execution_count": 7, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "part (a)\n", "material dispersion = 253.20 ns when h=850nm\n", "part (b)\n", "material dispersion = 6.72 ns when h=1300nm\n" ] } ], "source": [ "#pulse broadning\n", "print \"part (a)\"\n", "h=850##WAVELENGTH IN NANO METER\n", "l=80##fiber length in Km\n", "dh=30##in Nano Meter\n", "m1=105.5##material dispersion for h=850nm in ps/nm-Km\n", "m2=2.8##material dispersion for h=1300nm in ps/nm-Km\n", "t=m1*l*dh*10**-3##material dispersion in ns when h=850nm\n", "print \"material dispersion = %0.2f ns when h=850nm\"%t\n", "print \"part (b)\"\n", "h=1300##WAVELENGTH IN NANO METER\n", "l=80##fiber length in Km\n", "dh=30##in Nano Meter\n", "m1=105.5##material dispersion for h=850nm in ps/nm-Km\n", "m2=2.8##material dispersion for h=1300nm in ps/nm-Km\n", "t=m2*l*dh*10**-3##material dispersion in ns when h=850nm\n", "print \"material dispersion = %0.2f ns when h=1300nm\"%t" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 2.5 : Page 28" ] }, { "cell_type": "code", "execution_count": 9, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "part (a)\n", "material dispersion = 16.88 ns when h=850nm\n", "part (b)\n", "material dispersion = 0.448 ns when h=1300nm\n" ] } ], "source": [ "# pulse broadning\n", "print \"part (a)\"\n", "h=850##WAVELENGTH IN NANO METER\n", "l=80##fiber length in Km\n", "dh=2##in Nano Meter\n", "m1=105.5##material dispersion for h=850nm in ps/nm-Km\n", "m2=2.8##material dispersion for h=1300nm in ps/nm-Km\n", "t=m1*l*dh*10**-3##material dispersion in ns when h=850nm\n", "print \"material dispersion = %0.2f ns when h=850nm\"%t\n", "print \"part (b)\"\n", "h=1300##WAVELENGTH IN NANO METER\n", "l=80##fiber length in Km\n", "dh=2##in Nano Meter\n", "m1=105.5##material dispersion for h=850nm in ps/nm-Km\n", "m2=2.8##material dispersion for h=1300nm in ps/nm-Km\n", "t=m2*l*dh*10**-3##material dispersion in ns when h=850nm\n", "print \"material dispersion = %0.3f ns when h=1300nm\"%t" ] } ], "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 }