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author | Trupti Kini | 2016-03-06 23:30:10 +0600 |
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committer | Trupti Kini | 2016-03-06 23:30:10 +0600 |
commit | f78ea80ea8da9f42637ce019f233895e0638b230 (patch) | |
tree | 3ef9791b558642676567bf2b4dc94f9b38a57c31 /Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter3.ipynb | |
parent | 22e17d795629cfe00e03435f879cfd07f27e096a (diff) | |
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Added(A)/Deleted(D) following books
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter10.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter11.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter12.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter13.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter14.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter2.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter3.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter4.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter5.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter6.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter7.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter8.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter9.ipynb
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/screenshots/1.png
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/screenshots/2.png
A Fiber_Optics_and_Optoelectronics_by_R._P._Khare/screenshots/3.png
A sample_notebooks/LalitKumar/Ch3.ipynb
Diffstat (limited to 'Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter3.ipynb')
-rw-r--r-- | Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter3.ipynb | 226 |
1 files changed, 226 insertions, 0 deletions
diff --git a/Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter3.ipynb b/Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter3.ipynb new file mode 100644 index 00000000..9d40ec6f --- /dev/null +++ b/Fiber_Optics_and_Optoelectronics_by_R._P._Khare/Chapter3.ipynb @@ -0,0 +1,226 @@ +{ + "cells": [ + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "# Chapter3 - Wave propagation in planor waveguides" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example 3.1 : Page 45" + ] + }, + { + "cell_type": "code", + "execution_count": 1, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "range of propagation constant is 1.10880e+07 to 1.1014e+07 m**-1\n", + "number of modes are 4.0\n" + ] + } + ], + "source": [ + "from math import pi, sqrt\n", + "#range of propagation constants and maximum no. of modes\n", + "n1=1.5##core refractive index\n", + "n2=1.49##cladding refrative index\n", + "t=9.83##thickness of guided layer in micro meter\n", + "h=0.85##wavelength in µm\n", + "b1=((2*pi*n1)/(h*10**-6))##phase propagation constant in m**-1\n", + "b2=((2*pi*n2)/(h*10**-6))##phase propagation constant in m**-1\n", + "m=((4*t)/h)*(sqrt(n1**2-n2**2))##number of modes\n", + "print \"range of propagation constant is %0.5e\"%(b1),\" to %0.4e\"%(b2),\" m**-1\"\n", + "print\"number of modes are\",round(m/2)" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example 3.2 : Page 51" + ] + }, + { + "cell_type": "code", + "execution_count": 2, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "thicknes of the slab should not be greater than 0.794 µm\n" + ] + } + ], + "source": [ + "from math import sqrt\n", + "#thickness\n", + "n1=3.6##core refractive index\n", + "n2=3.56##cladding refrative index\n", + "h=0.85##wavelength in µm\n", + "a=((h/(2*sqrt(n1**2-n2**2))))##thickness in µm\n", + "print \"thicknes of the slab should not be greater than %0.3f\"%(a),\" µm\"" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example 3.3 : Page 52" + ] + }, + { + "cell_type": "code", + "execution_count": 3, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "part (a)\n", + "number of modes are : 5.0\n", + "part (b)\n", + "m \tuma(rad) \tum(m**-1) \twma(rad) \twm(m**-1) \tbm((wma/v)**2] \t\n", + "\n", + "0 1.30644 2.5845e+05 4.8263 9.5476e+05 0.93077\n", + "1 2.59574 5.1350e+05 4.27342 8.4538e+05 0.72974\n", + "2 3.83747 7.5914e+05 3.20529 6.3408e+05 0.41053\n", + "3 4.9063 9.7058e+05 0.963466 1.9060e+05 0.03709\n" + ] + } + ], + "source": [ + "from math import pi, sqrt\n", + "#no. of modes\n", + "print \"part (a)\"\n", + "n1=1.5##core refractive index\n", + "n2=1.48##cladding refrative index\n", + "t=10.11##thickness of guided layer in micro meter\n", + "h=1.55##wavelength in µm\n", + "b1=((2*pi*n1)/(h*10**-6))##phase propagation constant in m**-1\n", + "b2=((2*pi*n2)/(h*10**-6))##phase propagation constant in m**-1\n", + "m=((2*pi*t)/h)*(sqrt(n1**2-n2**2))##number of modes\n", + "print \"number of modes are : \",round(m/2)\n", + "\n", + "print \"part (b)\"\n", + "t1=10.11##thickness of guided layer in micro meter\n", + "t=t1/2#\n", + "h=1.55##wavelength in µm\n", + "b1=((2*pi*n1)/(h*10**-6))##phase propagation constant in m**-1\n", + "b2=((2*pi*n2)/(h*10**-6))##phase propagation constant in m**-1\n", + "mo=(((2*pi*t1)/h)*(sqrt(n1**2-n2**2)))/2##number of modes\n", + "uma0=1.30644## for m=0 from the curve\n", + "uma1=2.59574## for m=1 from the curve\n", + "uma2=3.83747## for m=2 from the curve\n", + "uma3=4.9063## for m=3 from the curve\n", + "wma0=4.8263## for m=0 from the curve\n", + "wma1=4.27342## for m=1 from the curve\n", + "wma2=3.20529## for m=2 from the curve\n", + "wma3=0.963466## for m=3 from the curve\n", + "um0=uma0/(t*10**-6)##in m**-1\n", + "um1=uma1/(t*10**-6)##in m**-1\n", + "um2=uma2/(t*10**-6)##in m**-1\n", + "um3=uma3/(t*10**-6)##in m**-1\n", + "wm0=wma0/(t*10**-6)##in m**-1\n", + "wm1=wma1/(t*10**-6)##in m**-1\n", + "wm2=wma2/(t*10**-6)##in m**-1\n", + "wm3=wma3/(t*10**-6)##in m**-1\n", + "bm0=((wm0*t*10**-6)/mo)**2##for m=0 \n", + "bm1=((wm1*t*10**-6)/mo)**2##for m=1\n", + "bm2=((wm2*t*10**-6)/mo)**2##for m=2 \n", + "bm3=((wm3*t*10**-6)/mo)**2##for m=3\n", + "m0=sqrt((bm0*(b1**2-b2**2))+b2**2)##for m=0 in m**-1\n", + "m1=sqrt((bm1*(b1**2-b2**2))+b2**2)##for m=1 in m**-1\n", + "m2=sqrt((bm2*(b1**2-b2**2))+b2**2)##for m=2 in m**-1\n", + "m3=sqrt((bm3*(b1**2-b2**2))+b2**2)##for m=3 in m**-1\n", + "params = [\"m\", \"uma(rad)\", \"um(m**-1)\", \"wma(rad)\", \"wm(m**-1)\", \"bm((wma/v)**2]\" ]\n", + "for x in params:\n", + " print x,'\\t',\n", + "\n", + "print '\\n'\n", + "a = range(0,4)\n", + "b = [uma0, uma1, uma2, uma3]\n", + "c = [um0, um1, um2, um3]\n", + "d = [wma0, wma1, wma2, wma3]\n", + "e = [wm0, wm1, wm2, wm3]\n", + "f = [bm0, bm1, bm2, bm3]\n", + "from numpy import nditer\n", + "for k,l,m,n,o,p in nditer([a,b,c,d,e,f]) :\n", + " print k,' ',l,' %0.4e'%m,' ',n,' %0.4e'%o,' %0.5f'%p\n" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example 3.4 : Page 56" + ] + }, + { + "cell_type": "code", + "execution_count": 4, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "G factor is 0.5622\n" + ] + } + ], + "source": [ + "from math import sin, cos, pi\n", + "#G factor\n", + "d=0.793##in micro meter\n", + "v=pi/2##point of intersection\n", + "ua=0.934##\n", + "wa=1.262##\n", + "Y=(wa*(1+(sin(ua*pi/180))*(cos(ua*pi/180))/ua))\n", + "G=(1+((cos(ua*pi/180))**2)/Y)**(-1)\n", + "print \"G factor is %0.4f\"%G\n", + "#answer is wrong in the textbook" + ] + } + ], + "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 +} |