{ "metadata": { "name": "", "signature": "sha256:c3f1cf4a5fa47c6ef9a25eb541b21d8b2dacc1e06513af0b6ceab3905b06fd91" }, "nbformat": 3, "nbformat_minor": 0, "worksheets": [ { "cells": [ { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "Chapter 12: Nonlinear effects" ] }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 12.1, Page Number: 432" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#variable declaration\n", "L = 75.0 #amplifier spcaing (kilometer)\n", "alpha = 4.61*10**-2 #fiber attenuation (per Km)\n", "\n", "#calculation\n", "Leff = (1-math.exp(-alpha*L))/alpha #effective length(km)\n", "\n", "#result\n", "print \"Effective length of fiber = \" , round(Leff,0) , \"km\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Effective length of fiber = 21.0 km\n" ] } ], "prompt_number": 1 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 12.2, Page Number: 433" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#variable declaration\n", "delta_VB = 20*10**6 #Brillouin linewidth (Hz)\n", "Aeff = 55*10**-12 #effective cross-sectional area of the propagating wave (square meter)\n", "Leff = 20*10**03 #effective length(km)\n", "b = 2 #polarization factor\n", "gB = 4*10**-11 #Brillous gain co-efficient (m/W)\n", "delta_Vsource = 40*10**6 #optical source linewidth (Hz)\n", "\n", "#calculation\n", "Pth = 21*(Aeff*b/(gB*Leff))*(1+(delta_Vsource/delta_VB)) #SBS threshold power(W)\n", "Ps_out_db = 10*(math.log10(Pth*10**3)) #SBS threshold power(dB)\n", "\n", "#result\n", "print \"SBS threshold power = \" , round(Pth*10**3,1) ,\"mW\"\n", "print \"SBS threshold power = \" , round(Ps_out_db,1) ,\"dBm\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "SBS threshold power = 8.7 mW\n", "SBS threshold power = 9.4 dBm\n" ] } ], "prompt_number": 2 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 12.3, Page Number: 438" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#variable declaration\n", "sus_P=6*10**-15 #Third order nonliner suseptibility (m^3/Ws)\n", "D = 3 #degenereting factor\n", "Leff = 22*10**03 #effective length (meters)\n", "Aeff = 6.4*10**-11 #effective cross-sectional area of the fiber (m^2)\n", "etta = 0.05 #quantum efficiency\n", "Lambda = 1540*10**-9 #Wavelength in single mode fibers (meters)\n", "C = 3*10**8 #free space velocity (m/s)\n", "alpha = 0.0461 #attenuation (per Km)\n", "L = 75 #fiberlink length (Km)\n", "P = 10**-3 #each channel input power of 1 mW\n", "n = 1.48 #refractive index\n", "\n", "#calculation\n", "k = ((32*(math.pi**3)*sus_P)/((n**2)*Lambda*C))*(Leff/Aeff) #nonlinear interaction constant\n", "P112 = etta*(D**2)*(k**2)*(P**3)*(math.exp(-alpha*L)) #power genreted(W)\n", "\n", "#result\n", "print \"Power genreted due to intrection of signals at different freqencies = \" , round(P112*10**11,2)*10**-8 , \"mW\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Power genreted due to intrection of signals at different freqencies = 5.8e-08 mW\n" ] } ], "prompt_number": 3 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 12.4, Page Number: 446" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#variable declaration \n", "Ts1 = 15*10**-12 #FWHM soliton pulse width\n", "Ts2 = 50*10**-12\n", "\n", "#calculation\n", "To1 = Ts1/1.7627 #normalized time(sec)\n", "To2 = Ts2/1.7627\n", "\n", "#result\n", "print \"Normalized time for FWHM soliton pulse = \" , round(To1*10**12) , \"-\" , round(To2*10**12+2) , \"ps\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Normalized time for FWHM soliton pulse = 9.0 - 30.0 ps\n" ] } ], "prompt_number": 4 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 12.5, Page Number: 446" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#variable declaration\n", "Ts = 20*10**-12 #FWHM soliton pulse width (sec) \n", "D = 0.5*10**-6 #dispersion of the fiber (ps/(nm*km))\n", "Lambda = 1550*10**-9 #wavelength (meter)\n", "C = 3*10**8 #free space velocity (m/s)\n", "\n", "#calculation\n", "Ldisp = 0.322*2*math.pi*C*(Ts**2)/((Lambda**2)*D) #dispersion length(Km)\n", "\n", "#result\n", "print \"Dispersion length = \" , round(Ldisp/1000) , \"Km\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Dispersion length = 202.0 Km\n" ] } ], "prompt_number": 5 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 12.6, Page Number: 447" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#variable declaration\n", "Lambda = 1550*10**-9 #wavelength (meters)\n", "n2 = 2.6*10**-20 #power (square m/w)\n", "Aeff = 50*10**-12 #effective area (m^2)\n", "Ldisp = 202*10**3 #dispersion length (meters)\n", "\n", "#calculation\n", "Ppeak = (Aeff/(2*math.pi*n2))*(Lambda/Ldisp) #soliton of peak power()\n", "\n", "#result\n", "print \"Soliton of peak power = \" , round(Ppeak*1000,2) , \"mW\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Soliton of peak power = 2.35 mW\n" ] } ], "prompt_number": 6 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 12.7, Page Number: 448" ] }, { "cell_type": "heading", "level": 3, "metadata": {}, "source": [ "Example 12.7(a)" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#variable declaration\n", "Ldisp = 100*10**03 #disperison length in m\n", "omega = 4682 #oscillation period\n", "\n", "#calculation\n", "LI = omega*Ldisp #interaction distance(km)\n", "\n", "#result\n", "print \"Interaction distance >= \" , round(LI*10**-5/1000,1) , \"e+05 km\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Interaction distance >= 4.7 e+05 km\n" ] } ], "prompt_number": 7 }, { "cell_type": "heading", "level": 3, "metadata": {}, "source": [ "Example 12.7(b)" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#variable declaration\n", "D = 0.5*10**-6 #disperison of fiber (ps/nm.km)\n", "C = 3*10**8 #free space velocity(m/s)\n", "S0 = 8 #normalized separation of neighnoring solitons\n", "B = 10*10**9 #data rate (10Gb/sec)\n", "Lambda = 1550*10**-9 #wavelength (m)\n", "\n", "#calculation\n", "Beta2 = (Lambda/(2*math.pi));\n", "LT = (C*math.exp(S0))/(16*D*B**2*(Beta2**2)*(S0**2)) #Total transmission distance(km)\n", "\n", "#result\n", "print \"Total transmission distance in km << \" , round(LT/10000),\"km\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Total transmission distance in km << 28701.0 km\n" ] } ], "prompt_number": 8 }, { "cell_type": "heading", "level": 3, "metadata": {}, "source": [ "Example 12.7(c), Page Number: 449" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#variable declaration\n", "S0 = 8 #normalized separation of neighnoring solitons\n", "B = 10*10**9 #data rate (10Gb/sec)\n", "\n", "#calculation\n", "Ts = 0.881/(S0*B) #FHWM soliton pulse width\n", "\n", "#result\n", "print \"FWHM soliton pulse width = \" , round(Ts*1000*10**9),\"ps\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "FWHM soliton pulse width = 11.0 ps\n" ] } ], "prompt_number": 9 }, { "cell_type": "heading", "level": 3, "metadata": {}, "source": [ "Example 12.7(d), Page Number: 449" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "\n", "#variable declaration\n", "S0 = 8 #normalized separation of neighnoring solitons\n", "\n", "#calculation \n", "Ts_TB = 0.881/S0 #fraction of bit slot occupied by a soliton\n", "\n", "#result\n", "print \"Fraction of bit slot occupied by a soliton in % = \" , round(Ts_TB*100),\"%\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Fraction of bit slot occupied by a soliton in % = 11.0 %\n" ] } ], "prompt_number": 10 } ], "metadata": {} } ] }