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author | Thomas Stephen Lee | 2015-09-04 22:04:10 +0530 |
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committer | Thomas Stephen Lee | 2015-09-04 22:04:10 +0530 |
commit | 41f1f72e9502f5c3de6ca16b303803dfcf1df594 (patch) | |
tree | f4bf726a3e3ce5d7d9ee3781cbacfe3116115a2c /Applied_Physics_II/Chapter_3.ipynb | |
parent | 9c9779ba21b9bedde88e1e8216f9e3b4f8650b0e (diff) | |
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diff --git a/Applied_Physics_II/Chapter_3.ipynb b/Applied_Physics_II/Chapter_3.ipynb deleted file mode 100755 index 61c99435..00000000 --- a/Applied_Physics_II/Chapter_3.ipynb +++ /dev/null @@ -1,779 +0,0 @@ -{ - "metadata": { - "name": "" - }, - "nbformat": 3, - "nbformat_minor": 0, - "worksheets": [ - { - "cells": [ - { - "cell_type": "heading", - "level": 1, - "metadata": {}, - "source": [ - "Chapter 3: Fibre Optics" - ] - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.3.1, Page number 3-6" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n1 = 1.54 #refractive index of core\n", - "NA = 0.5 #numerical aperture\n", - "\n", - "#Calculation\n", - "n2 = math.sqrt(n1**2-NA**2)\n", - "\n", - "#Result\n", - "print \"Refractive index of cladding is\",round(n2,2)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Refractive index of cladding is 1.46\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.3.2, Page number 3-6" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n2 = 1.59 #refractive index of cladding\n", - "NA = 0.2 #numerical aperture\n", - "n0 = 1.33\n", - "\n", - "#Calculation\n", - "n1 = (math.sqrt(n2**2-NA**2))\n", - "theta_o = (math.asin((math.sqrt(n2**2-n1**2)/n0)))*180/math.pi\n", - "\n", - "#Result\n", - "print \"Refractive index of core is\",n2\n", - "print \"Acceptance angle =\",round(theta_o,2),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Refractive index of core is 1.59\n", - "Acceptance angle = 8.65 degrees\n" - ] - } - ], - "prompt_number": 1 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.3.3, Page number 3-6\n" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n1 = 1.49 #refractive index of core\n", - "n2 = 1.44 #refractive index of cladding\n", - "\n", - "#Calculation\n", - "NA = math.sqrt(n1**2-n2**2)\n", - "\n", - "theta_o = math.degrees(math.asin(NA))\n", - "\n", - "#Result\n", - "print \"Numerical Aperture =\",round(NA,5)\n", - "print \"Acceptance angle =\",round(theta_o,2),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Numerical Aperture = 0.38275\n", - "Acceptance angle = 22.5 degrees\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.3.4, Page number 3-7" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n1 = 1.6 #refractive index of core\n", - "n2 = 1.3 #refractive index of cladding\n", - "\n", - "#Calculation\n", - "theta_c = math.degrees(math.asin(n2/n1))\n", - "\n", - "theta_o = math.degrees(math.asin(math.sqrt(n1**2-n2**2)))\n", - "AC = 2*theta_o\n", - "\n", - "#Result\n", - "print \"Critical angle =\",round(theta_c,2),\"degrees\"\n", - "print \"Value of angle of acceptance cone =\",round(AC,3),\"degrees\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Critical angle = 54.34 degrees\n", - "Value of angle of acceptance cone = 137.731 degrees\n" - ] - } - ], - "prompt_number": 1 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.3.5, Page number 3-7" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n1 = 1.4 #refractive index of core\n", - "theta_o = 30 #acceptance angle(degrees)\n", - "\n", - "#Calculation\n", - "n2 = math.sqrt(n1**2-math.sin(math.radians(theta_o))**2)\n", - "\n", - "#Result\n", - "print \"Refractive index of cladding is\",round(n2,4)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Refractive index of cladding is 1.3077\n" - ] - } - ], - "prompt_number": 11 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.3.6, Page number 3-8" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "#Variable declaration\n", - "n1 = 1.563 #refractive index of core\n", - "n2 = 1.498 #refractive index of cladding\n", - "\n", - "#Calculation\n", - "delta = (n1-n2)/n1\n", - "\n", - "#Result\n", - "print \"Fractional index change =\",round(delta,4)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Fractional index change = 0.0416\n" - ] - } - ], - "prompt_number": 26 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.3.7, Page number 3-8" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "#Variable declaration\n", - "n1 = 1.50 #refractive index of cladding\n", - "theta_c = 90-5 #critical angle(degrees)\n", - "\n", - "#Calculation\n", - "n2 = math.sin(theta_c*math.pi/180)*n1\n", - "\n", - "#Result\n", - "print \"The maximum index of refraction allowed for cladding is\",round(n2,4)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "The maximum index of refraction allowed for cladding is 1.4943\n" - ] - } - ], - "prompt_number": 28 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.3.8, Page number 3-8" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "#Variable declaration\n", - "n1 = 1.33 #refractive index \n", - "theta_o = 30 #acceptance angle in air\n", - "\n", - "#Calculations\n", - "theta_0 = math.degrees(math.asin(math.sin(theta_o*math.pi/180)/n1))\n", - "\n", - "#Result\n", - "print \"Acceptance angle =\",round(theta_0,2),\"degrees\"\n" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Acceptance angle = 22.08 degrees\n" - ] - } - ], - "prompt_number": 36 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.4.1, Page number 3-10" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n1 = 1.52 #refractive index of core\n", - "n2 = 1.5189 #refractive index of cladding\n", - "d = 29*10**-6 #core diameter(m)\n", - "lamda = 1.3*10**-6 #wavelength(m)\n", - "\n", - "#Calculation\n", - "V = (math.pi*d*math.sqrt(n1**2-n2**2))/lamda\n", - "\n", - "N = V**2/2\n", - "\n", - "#Results\n", - "print \"Normalized frequency =\",round(V,3)\n", - "print \"Number of modes =\",round(N)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Normalized frequency = 4.052\n", - "Number of modes = 8.0\n" - ] - } - ], - "prompt_number": 40 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.4.2, Page number 3-10" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n1 = 1.47 #refractive index of core\n", - "n2 = 1.46 #refractive index of cladding\n", - "lamda = 1300*10**-9 #wavelength(nm)\n", - "V = 2.405 #for single mode fibre\n", - "\n", - "#Calculation\n", - "d = (V*lamda)/(math.pi*math.sqrt(n1**2-n2**2))\n", - "r = d/2\n", - "\n", - "#Result\n", - "print \"Radius =\",round(r/1e-6,3),\"um\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Radius = 2.907 um\n" - ] - } - ], - "prompt_number": 48 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.4.3, Page number 3-11" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n1 = 1.48 #refractive index of core\n", - "delta = 0.055 #relative RI\n", - "lamda = 1 #wavelength(um)\n", - "r = 50 #core radius(um)\n", - "\n", - "#Calculations\n", - "n2 = -((delta*n1)-n1)\n", - "\n", - "NA = math.sqrt(n1**2-n2**2)\n", - "\n", - "theta_o = math.degrees(math.asin(NA))\n", - "\n", - "V = (math.pi*2*r*NA)/lamda\n", - "\n", - "N = V**2/2\n", - "\n", - "#Results\n", - "print \"Refractive index of cladding =\",n2\n", - "print \"NA =\",round(NA,3)\n", - "print \"Acceptance angle =\",round(theta_o,2),\"degrees\"\n", - "print \"Normalized frequency =\",round(V,3)\n", - "print \"Number of modes =\",round(N) #Answer differs due to rounding off in 'V'" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Refractive index of cladding = 1.3986\n", - "NA = 0.484\n", - "Acceptance angle = 28.95 degrees\n", - "Normalized frequency = 152.073\n", - "Number of modes = 11563.0\n" - ] - } - ], - "prompt_number": 13 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.4.4, Page number 3-12" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n1 = 1.45 #refractive index of core\n", - "n2 = 1.448 #refractive index of cladding\n", - "lamda = 1*10**-6 #wavelength(m)\n", - "d = 6*10**-6 #core diameter(m)\n", - "\n", - "#Calculations\n", - "#Case i\n", - "theta_c = math.degrees(math.asin(n2/n1))\n", - "\n", - "#Case ii\n", - "theta_o = math.degrees(math.asin(math.sqrt(n1**2-n2**2)))\n", - "\n", - "#Case iii\n", - "NA = math.sqrt(n1**2-n2**2)\n", - "N = (math.pi**2*d**2*NA**2)/(2*lamda**2)\n", - "\n", - "#Results\n", - "print \"Critical angle =\",round(theta_c),\"degrees\"\n", - "print \"Acceptance angle =\",round(theta_o,3),\"degrees\"\n", - "print \"Number of modes =\",round(N)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Critical angle = 87.0 degrees\n", - "Acceptance angle = 4.366 degrees\n", - "Number of modes = 1.0\n" - ] - } - ], - "prompt_number": 2 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.4.5, Page number 3-12" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n1 = 1.50 #refractive index of core\n", - "n2 = 1.48 #refractive index of cladding\n", - "lamda = 1*10**-6 #wavelength(m)\n", - "d = 2*50*10**-6 #core diameter(m)\n", - "\n", - "#Calculations\n", - "NA = math.sqrt(n1**2-n2**2)\n", - "N = (math.pi**2*d**2*NA**2)/(2*lamda**2)\n", - "\n", - "#Result\n", - "print \"Number of modes =\",round(N)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Number of modes = 2941.0\n" - ] - } - ], - "prompt_number": 3 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.4.6, Page number 3-13" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "n1 = 1.55 #refractive index of core\n", - "n2 = 1.50 #refractive index of cladding\n", - "lamda = 1400*10**-9 #wavelength(m)\n", - "d = 40*10**-6 #core diameter(m)\n", - "\n", - "#Calculations\n", - "NA = math.sqrt(n1**2-n2**2)\n", - "\n", - "delta = (n1-n2)/n1\n", - "\n", - "V = (math.pi*d*NA)/lamda\n", - "\n", - "#Results\n", - "print \"NA =\",round(NA,4)\n", - "print \"Fractional index change =\",round(delta,5)\n", - "print \"V-number =\",round(V,2)" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "NA = 0.3905\n", - "Fractional index change = 0.03226\n", - "V-number = 35.05\n" - ] - } - ], - "prompt_number": 4 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.6.1, Page number 3-17" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "Pout = 0.3 #output power(mW)\n", - "Pin = 1 #input power(mW)\n", - "L = 0.1 #fibre length(km)\n", - "\n", - "#Calculation\n", - "a = (-10/L)*math.log10(Pout/Pin)\n", - "\n", - "#Result\n", - "print \"Attenuation =\",round(a,2),\"dB/km\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Attenuation = 52.29 dB/km\n" - ] - } - ], - "prompt_number": 5 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.6.2, Page number 3-18" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "import math\n", - "\n", - "#Variable declaration\n", - "Pin = 9 #input power(mW)\n", - "L = 3 #fibre length(km)\n", - "a = 1.5 #loss(dB/km)\n", - "\n", - "#Calculation\n", - "Pl = a*L\n", - "Pout = Pin*10**(-Pl/10)\n", - "\n", - "#Result\n", - "print \"Output power =\",round(Pout,3),\"uW\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Output power = 3.193 uW\n" - ] - } - ], - "prompt_number": 12 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.6.3, Page number 3-18" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "#Variable declaration\n", - "a = 2.2 #attenuation(dB/km)\n", - "l1 = 2 #km\n", - "l2 = 6 #km\n", - "from sympy import * \n", - "Pin = symbols('Pin')\n", - "\n", - "#Calculations\n", - "#For 2km,\n", - "Pl1 = a*l1\n", - "Po1 = Pin*round(10**(-Pl1/10),3)\n", - "\n", - "#For 6km,\n", - "Pl2 = a*l2\n", - "Po2 = Pin*round(10**(-Pl2/10),3)\n", - "\n", - "#Results\n", - "print \"After 2 km, Pout =\",Po1\n", - "print \"After 6 km, Pout =\",Po2" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "After 2 km, Pout = 0.363*Pin\n", - "After 6 km, Pout = 0.048*Pin\n" - ] - } - ], - "prompt_number": 17 - }, - { - "cell_type": "heading", - "level": 2, - "metadata": {}, - "source": [ - "Example 3.6.4, Page number 3-19" - ] - }, - { - "cell_type": "code", - "collapsed": false, - "input": [ - "\n", - "#Variable declaration\n", - "Pout = 7.5 #output power(mW)\n", - "Pin = 8.6 #input power(mW)\n", - "L = 0.5 #fibre length(km)\n", - "\n", - "#Calculation\n", - "Pl = -10*math.log10(Pout/Pin)\n", - "a = Pl/L\n", - "\n", - "#Result\n", - "print \"Loss specification =\",round(a,4),\"dB/km\"" - ], - "language": "python", - "metadata": {}, - "outputs": [ - { - "output_type": "stream", - "stream": "stdout", - "text": [ - "Loss specification = 1.1887 dB/km\n" - ] - } - ], - "prompt_number": 19 - } - ], - "metadata": {} - } - ] -}
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