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author | debashisdeb | 2014-06-20 15:42:42 +0530 |
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committer | debashisdeb | 2014-06-20 15:42:42 +0530 |
commit | 83c1bfceb1b681b4bb7253b47491be2d8b2014a1 (patch) | |
tree | f54eab21dd3d725d64a495fcd47c00d37abed004 /Elements_of_Electromagnetics/chapter_12.ipynb | |
parent | a78126bbe4443e9526a64df9d8245c4af8843044 (diff) | |
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removing problem statements
Diffstat (limited to 'Elements_of_Electromagnetics/chapter_12.ipynb')
-rw-r--r-- | Elements_of_Electromagnetics/chapter_12.ipynb | 869 |
1 files changed, 418 insertions, 451 deletions
diff --git a/Elements_of_Electromagnetics/chapter_12.ipynb b/Elements_of_Electromagnetics/chapter_12.ipynb index b6ded6a6..e098f292 100644 --- a/Elements_of_Electromagnetics/chapter_12.ipynb +++ b/Elements_of_Electromagnetics/chapter_12.ipynb @@ -1,452 +1,419 @@ -{
- "metadata": {
- "name": "chapter_12.ipynb"
- },
- "nbformat": 3,
- "nbformat_minor": 0,
- "worksheets": [
- {
- "cells": [
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h1>Chapter 12: Waveguides<h1>"
- ]
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 12.1, Page number: 557<h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "from __future__ import division\n",
- "'''\n",
- "A rectangular waveguide with dimensions a = 2.5 cm, b = 1 cm is to \n",
- "operate below 15.1 GHz. How many TE and TM modes can the waveguide transmit\n",
- "if the guide is filled with a medium characterized by sigma = 0, epsilon = 4\n",
- "epsilon_o,mu_r = 1? Calculate the cutoff frequencies of the modes. '''\n",
- "\n",
- "import scipy\n",
- "\n",
- "#Variable Declaration\n",
- "\n",
- "a=2.5*10**-2 #in m\n",
- "b=1*10**-2 #in m\n",
- "c=0\n",
- "Ur=1 #relative permeability\n",
- "Er=4 #relative permittivity\n",
- "C=3*10**8 #speed of wave in m/s\n",
- "fc=0\n",
- "m=0\n",
- "n=0\n",
- "\n",
- "#Calculations\n",
- "\n",
- "while (fc*10**-9 < 15.1) :\n",
- " fc = (C/(4*a))*scipy.sqrt(m**2+(a*n/b)**2)\n",
- " if (( fc*10**-9) < 15.1) :\n",
- " n=n+1\n",
- " else:\n",
- " print 'Maximum value of n is ',n-1\n",
- "\n",
- "nmax=n-1 \n",
- "fc=0\n",
- "m=0\n",
- "n=0\n",
- "while(fc*10**-9 < 15.1):\n",
- " fc =(C/(4*a))*scipy.sqrt(m**2+(a*n/b)**2)\n",
- " if((fc*10**-9) < 15.1):\n",
- " m=m+1\n",
- " else:\n",
- " print 'Maximum value of m is ',m-1 \n",
- "\n",
- "mmax=m-1\n",
- "m=0\n",
- "while(m<mmax+1):\n",
- " n=0\n",
- " while(n<nmax+1):\n",
- " p=(C/(4*a))*scipy.sqrt(m**2+(a*n/b)**2)\n",
- " if((p*10**-9) < 15.1) :\n",
- " print m,n,'transmission mode is possible'\n",
- " print 'frequency is',round(p*10**-9,2),'GHz'\n",
- " else:\n",
- " print m,n,'transmission mode is not possible'\n",
- " n=n+1\n",
- " \n",
- " m=m+1\n",
- " "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "Maximum value of n is 2\n",
- "Maximum value of m is 5\n",
- "0 0 transmission mode is possible\n",
- "frequency is 0.0 GHz\n",
- "0 1 transmission mode is possible\n",
- "frequency is 7.5 GHz\n",
- "0 2 transmission mode is possible\n",
- "frequency is 15.0 GHz\n",
- "1 0 transmission mode is possible\n",
- "frequency is 3.0 GHz\n",
- "1 1 transmission mode is possible\n",
- "frequency is 8.08 GHz\n",
- "1 2 transmission mode is not possible\n",
- "2 0 transmission mode is possible\n",
- "frequency is 6.0 GHz\n",
- "2 1 transmission mode is possible\n",
- "frequency is 9.6 GHz\n",
- "2 2 transmission mode is not possible\n",
- "3 0 transmission mode is possible\n",
- "frequency is 9.0 GHz\n",
- "3 1 transmission mode is possible\n",
- "frequency is 11.72 GHz\n",
- "3 2 transmission mode is not possible\n",
- "4 0 transmission mode is possible\n",
- "frequency is 12.0 GHz\n",
- "4 1 transmission mode is possible\n",
- "frequency is 14.15 GHz\n",
- "4 2 transmission mode is not possible\n",
- "5 0 transmission mode is possible\n",
- "frequency is 15.0 GHz\n",
- "5 1 transmission mode is not possible\n",
- "5 2 transmission mode is not possible\n"
- ]
- }
- ],
- "prompt_number": 1
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 12.3, Page number: 561<h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "'''\n",
- "In a rectangular waveguide for which a = 1.5 cm, b = 0.8 cm, sigma = 0, \n",
- "mu = mu_o and epsilon = 4epsilon_o,\n",
- "\n",
- "Hx=2sin(pi x/a) cos(3pi y/b)sin(pi X 10^11t - Bz) A/m\n",
- "\n",
- "Determine \n",
- "(a) The mode of operation \n",
- "(b) The cutoff frequency \n",
- "(c) The phase constant B \n",
- "(d) The propagation constant gamma\n",
- "(e) The intrinsic wave impedance eta '''\n",
- "\n",
- "import scipy\n",
- "import cmath\n",
- "from numpy import *\n",
- "\n",
- "#Variable Declaration\n",
- "\n",
- "a=1.5*10**-2 #in m\n",
- "b=0.8*10**-2 #in m\n",
- "c=0\n",
- "Uo=4*scipy.pi*10**-7 #permeability of free space\n",
- "Ur=1 #relative permeability\n",
- "Eo=10**-9/(36*scipy.pi) #permittivity of free space\n",
- "Er=4 #relative permittivity\n",
- "C=3*10**8 #speed of light in m/s\n",
- "w=scipy.pi*10**11 #omega in rad/s\n",
- "m=1\n",
- "n=3\n",
- "u=C/2 #speed of wave in m/s\n",
- "\n",
- "#Calculations\n",
- "\n",
- "f=w/(2*scipy.pi) #frequency of wave in Hz\n",
- "fc=u*((m*m)/(a*a)+(n*n)/(b*b))**0.5/2 #cutoff frequency in Hz\n",
- "B=w*scipy.sqrt(1-(fc/f)**2)/u #phase constant in rad/m\n",
- "eta=377/scipy.sqrt(Er)*scipy.sqrt(1-(fc/f)**2) #intrinsic wave impedance in ohm\n",
- "\n",
- "#Results\n",
- "\n",
- "print 'The cutoff frequency =',round(fc*10**-9,2),'GHz'\n",
- "print 'The phase constant =',round(B,2),'rad/m'\n",
- "print 'The propagation constant =',round(B,2),'j /m'\n",
- "print 'The intrinsic wave impedance =',round(eta,1),'ohms'"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "The cutoff frequency = 28.57 GHz\n",
- "The phase constant = 1718.93 rad/m\n",
- "The propagation constant = 1718.93 j /m\n",
- "The intrinsic wave impedance = 154.7 ohms\n"
- ]
- }
- ],
- "prompt_number": 2
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 12.4, Page number: 565<h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "'''\n",
- "A standard air-filled rectangular waveguide with dimensions a = 8.636 cm,\n",
- "b = 4.318 cm is fed by a 4-GHz carrier from a coaxial cable. Determine if a \n",
- "TE_10 mode will be propagated. If so, calculate the phase velocity and \n",
- "the group velocity. '''\n",
- "\n",
- "import scipy\n",
- "\n",
- "#Variable Declaration\n",
- "\n",
- "a=8.636*10**-2 #in m\n",
- "b=4.318*10**-2 #in m\n",
- "f=4*10**9 #in Hz\n",
- "u=3*10**8 #speed of wave in m/s\n",
- "\n",
- "#Calculations\n",
- "\n",
- "fc=u/(2*a)\n",
- "if(f>fc):\n",
- " print 'As f>fc, TE10 mode will propogate'\n",
- "else:\n",
- " print 'It will not propogate'\n",
- "\n",
- "Up=u/scipy.sqrt(1-(fc/f)**2) #phase velocity in m/s\n",
- "Ug=u*u/Up #group velocity in m/s\n",
- "\n",
- "#Results\n",
- "\n",
- "print 'Phase velocity =',round(Up*10**-6,0),'Mm/s'\n",
- "print 'Group velocity =',round(Ug*10**-6,1),'Mm/s'"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "As f>fc, TE10 mode will propogate\n",
- "Phase velocity = 333.0 Mm/s\n",
- "Group velocity = 270.2 Mm/s\n"
- ]
- }
- ],
- "prompt_number": 3
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 12.5, Page number: 570<h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "'''\n",
- "An air-filled rectangular waveguide of dimensions a = 4 cm, b = 2 cm \n",
- "transports energy in the dominant mode at a rate of 2 mW. If the frequency of\n",
- "operation is lO GHz. Determine the peak value of the electric field \n",
- "in the waveguide. '''\n",
- "\n",
- "import scipy\n",
- "\n",
- "#Variable Declaration\n",
- "\n",
- "f=10*10**9 #frequency of operation in Hz\n",
- "a=4*10**-2 #in m\n",
- "b=2*10**-2 #in m\n",
- "u=3*10**8 #velocity in m/s\n",
- "Pavg=2*10**-3 #average power in W\n",
- "\n",
- "#Calculations\n",
- "\n",
- "fc=u/(2*a) #cutoff frequency in Hz\n",
- "n=377/scipy.sqrt(1-(fc/f)**2) #intrinsic wave impedance in ohms\n",
- "E=scipy.sqrt(4*n*Pavg/(a*b)) #peak value of electric field in V/m\n",
- "\n",
- "#Result\n",
- "\n",
- "print 'Peak value of electric field =',round(E,2),'V/m'"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "Peak value of electric field = 63.77 V/m\n"
- ]
- }
- ],
- "prompt_number": 4
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 12.6, Page number: 571<h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "'''\n",
- "A copper-plated waveguide (sigma_e = 5.8 X 10 7 S/m) operating at 4.8 GHz \n",
- "is supposed to deliver a minimum power of 1.2 kW to an antenna. If the guide\n",
- "is fillcd with polystyrene (sigma = 10^17 S/m, epsilon = 2.55 epsilon_o) and\n",
- "its dimensions are a = 4.2 cm, b = 2.6 cm, calculate the power dissipated in \n",
- "a length 60 cm of the guide in the TE_10 mode. '''\n",
- "\n",
- "import scipy\n",
- "\n",
- "#Variable declaration\n",
- "\n",
- "cc=5.8*10**7 #in S/m\n",
- "f=4.8*10**9 #in Hz\n",
- "c=10**-17 #in S/m\n",
- "Uo=4*scipy.pi*10**-7 #permeability of free space\n",
- "Eo=10**-9/(36*scipy.pi) #permittivity of free space\n",
- "Er=2.55 #relative permittivity\n",
- "z=60*10**-2 #in m\n",
- "l=4.2*10**-2 #in m\n",
- "b=2.6*10**-2 #in m\n",
- "P=1.2*10**3 #in W\n",
- "\n",
- "#Calculations\n",
- "\n",
- "n=377/scipy.sqrt(Er)\n",
- "u=3*10**8/scipy.sqrt(Er)\n",
- "fc=u/(2*l)\n",
- "ad=c*n/(2*scipy.sqrt(1-(fc/f)**2))\n",
- "Rs=scipy.sqrt(scipy.pi*f*Uo/cc)\n",
- "ac=2*Rs*(0.5+(b/l)*(fc/f)**2)/(b*n*scipy.sqrt(1-(fc/f)**2))\n",
- "a=ac\n",
- "Pd=P*(scipy.e**(2*a*z)-1)\n",
- "\n",
- "#Result\n",
- "\n",
- "print 'power dissipated =',round(Pd,3),'W'\n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "power dissipated = 6.096 W\n"
- ]
- }
- ],
- "prompt_number": 5
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 12.8, Page number: 579<h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "'''\n",
- "An air-filled resonant cavity with dimensions a = 5 cm, b = 4 cm, and \n",
- "c = 10 cm is made of copper (sigma_e = 5.8 X 10^7 mhos/m). Find \n",
- "(a) The five lowest order modes \n",
- "(b) The quality factor for TE_101 mode '''\n",
- "\n",
- "import scipy\n",
- "\n",
- "#Variable Declaration\n",
- " \n",
- "a=5*10**-2 #in m\n",
- "b=4*10**-2 #in m\n",
- "c=10*10**-2 #in m\n",
- "C=5.8*10**7 #in mhos/m\n",
- "Uo=4*scipy.pi*10**-7 #permeability of free space\n",
- "u=3*10**8 #speed of wave in m/s\n",
- "\n",
- "#Calculations\n",
- "\n",
- "def f(m,n,p):\n",
- " fr=scipy.sqrt((m/a)**2+(n/b)**2+(p/c)**2)*u/2 #resonant frequency in Hz\n",
- " print round(fr*10**-9,3)\n",
- " \n",
- "\n",
- "f101=3.35*10**9\n",
- "d=scipy.sqrt(1/(scipy.pi*f101*Uo*C))\n",
- "Q=(a*a+c*c)*a*b*c/(d*(2*b*(a**3+c**3)+a*c*(a*a+c*c))) #quality factor\n",
- "\n",
- "#Results\n",
- "\n",
- "print 'Thus the five lowest order modes in ascending order are '\n",
- "print 'TE101, frequency in GHz ='\n",
- "f(1,0,1)\n",
- "print 'TE011, frequency in GHz ='\n",
- "f(0,1,1)\n",
- "print 'TE102, frequency in GHz ='\n",
- "f(1,0,2)\n",
- "print 'TE110, frequency in GHz ='\n",
- "f(1,1,0)\n",
- "print 'TE111 or TM111, frequency in GHz ='\n",
- "f(1,1,1)\n",
- "print 'Quality factor =',round(Q,0)"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "Thus the five lowest order modes in ascending order are \n",
- "TE101, frequency in GHz =\n",
- "3.354\n",
- "TE011, frequency in GHz =\n",
- "4.039\n",
- "TE102, frequency in GHz =\n",
- "4.243\n",
- "TE110, frequency in GHz =\n",
- "4.802\n",
- "TE111 or TM111, frequency in GHz =\n",
- "5.031\n",
- "Quality factor = 14358.0\n"
- ]
- }
- ],
- "prompt_number": 6
- }
- ],
- "metadata": {}
- }
- ]
+{ + "metadata": { + "name": "", + "signature": "sha256:7e2f43e6e0f517c2aac74f69be1d132b3ab84b5c247c20e556eb69dbe9aedae5" + }, + "nbformat": 3, + "nbformat_minor": 0, + "worksheets": [ + { + "cells": [ + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "<h1>Chapter 12: Waveguides<h1>" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "<h3>Example 12.1, Page number: 557<h3>" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "from __future__ import division\n", + " \n", + "\n", + "import scipy\n", + "\n", + "#Variable Declaration\n", + "\n", + "a=2.5*10**-2 #in m\n", + "b=1*10**-2 #in m\n", + "c=0\n", + "Ur=1 #relative permeability\n", + "Er=4 #relative permittivity\n", + "C=3*10**8 #speed of wave in m/s\n", + "fc=0\n", + "m=0\n", + "n=0\n", + "\n", + "#Calculations\n", + "\n", + "while (fc*10**-9 < 15.1) :\n", + " fc = (C/(4*a))*scipy.sqrt(m**2+(a*n/b)**2)\n", + " if (( fc*10**-9) < 15.1) :\n", + " n=n+1\n", + " else:\n", + " print 'Maximum value of n is ',n-1\n", + "\n", + "nmax=n-1 \n", + "fc=0\n", + "m=0\n", + "n=0\n", + "while(fc*10**-9 < 15.1):\n", + " fc =(C/(4*a))*scipy.sqrt(m**2+(a*n/b)**2)\n", + " if((fc*10**-9) < 15.1):\n", + " m=m+1\n", + " else:\n", + " print 'Maximum value of m is ',m-1 \n", + "\n", + "mmax=m-1\n", + "m=0\n", + "while(m<mmax+1):\n", + " n=0\n", + " while(n<nmax+1):\n", + " p=(C/(4*a))*scipy.sqrt(m**2+(a*n/b)**2)\n", + " if((p*10**-9) < 15.1) :\n", + " print m,n,'transmission mode is possible'\n", + " print 'frequency is',round(p*10**-9,2),'GHz'\n", + " else:\n", + " print m,n,'transmission mode is not possible'\n", + " n=n+1\n", + " \n", + " m=m+1\n", + " " + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "Maximum value of n is 2\n", + "Maximum value of m is 5\n", + "0 0 transmission mode is possible\n", + "frequency is 0.0 GHz\n", + "0 1 transmission mode is possible\n", + "frequency is 7.5 GHz\n", + "0 2 transmission mode is possible\n", + "frequency is 15.0 GHz\n", + "1 0 transmission mode is possible\n", + "frequency is 3.0 GHz\n", + "1 1 transmission mode is possible\n", + "frequency is 8.08 GHz\n", + "1 2 transmission mode is not possible\n", + "2 0 transmission mode is possible\n", + "frequency is 6.0 GHz\n", + "2 1 transmission mode is possible\n", + "frequency is 9.6 GHz\n", + "2 2 transmission mode is not possible\n", + "3 0 transmission mode is possible\n", + "frequency is 9.0 GHz\n", + "3 1 transmission mode is possible\n", + "frequency is 11.72 GHz\n", + "3 2 transmission mode is not possible\n", + "4 0 transmission mode is possible\n", + "frequency is 12.0 GHz\n", + "4 1 transmission mode is possible\n", + "frequency is 14.15 GHz\n", + "4 2 transmission mode is not possible\n", + "5 0 transmission mode is possible\n", + "frequency is 15.0 GHz\n", + "5 1 transmission mode is not possible\n", + "5 2 transmission mode is not possible\n" + ] + } + ], + "prompt_number": 1 + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "<h3>Example 12.3, Page number: 561<h3>" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + " \n", + "import scipy\n", + "import cmath\n", + "from numpy import *\n", + "\n", + "#Variable Declaration\n", + "\n", + "a=1.5*10**-2 #in m\n", + "b=0.8*10**-2 #in m\n", + "c=0\n", + "Uo=4*scipy.pi*10**-7 #permeability of free space\n", + "Ur=1 #relative permeability\n", + "Eo=10**-9/(36*scipy.pi) #permittivity of free space\n", + "Er=4 #relative permittivity\n", + "C=3*10**8 #speed of light in m/s\n", + "w=scipy.pi*10**11 #omega in rad/s\n", + "m=1\n", + "n=3\n", + "u=C/2 #speed of wave in m/s\n", + "\n", + "#Calculations\n", + "\n", + "f=w/(2*scipy.pi) #frequency of wave in Hz\n", + "fc=u*((m*m)/(a*a)+(n*n)/(b*b))**0.5/2 #cutoff frequency in Hz\n", + "B=w*scipy.sqrt(1-(fc/f)**2)/u #phase constant in rad/m\n", + "eta=377/scipy.sqrt(Er)*scipy.sqrt(1-(fc/f)**2) #intrinsic wave impedance in ohm\n", + "\n", + "#Results\n", + "\n", + "print 'The cutoff frequency =',round(fc*10**-9,2),'GHz'\n", + "print 'The phase constant =',round(B,2),'rad/m'\n", + "print 'The propagation constant =',round(B,2),'j /m'\n", + "print 'The intrinsic wave impedance =',round(eta,1),'ohms'" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The cutoff frequency = 28.57 GHz\n", + "The phase constant = 1718.93 rad/m\n", + "The propagation constant = 1718.93 j /m\n", + "The intrinsic wave impedance = 154.7 ohms\n" + ] + } + ], + "prompt_number": 2 + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "<h3>Example 12.4, Page number: 565<h3>" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + " \n", + "import scipy\n", + "\n", + "#Variable Declaration\n", + "\n", + "a=8.636*10**-2 #in m\n", + "b=4.318*10**-2 #in m\n", + "f=4*10**9 #in Hz\n", + "u=3*10**8 #speed of wave in m/s\n", + "\n", + "#Calculations\n", + "\n", + "fc=u/(2*a)\n", + "if(f>fc):\n", + " print 'As f>fc, TE10 mode will propogate'\n", + "else:\n", + " print 'It will not propogate'\n", + "\n", + "Up=u/scipy.sqrt(1-(fc/f)**2) #phase velocity in m/s\n", + "Ug=u*u/Up #group velocity in m/s\n", + "\n", + "#Results\n", + "\n", + "print 'Phase velocity =',round(Up*10**-6,0),'Mm/s'\n", + "print 'Group velocity =',round(Ug*10**-6,1),'Mm/s'" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "As f>fc, TE10 mode will propogate\n", + "Phase velocity = 333.0 Mm/s\n", + "Group velocity = 270.2 Mm/s\n" + ] + } + ], + "prompt_number": 3 + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "<h3>Example 12.5, Page number: 570<h3>" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + " \n", + "\n", + "import scipy\n", + "\n", + "#Variable Declaration\n", + "\n", + "f=10*10**9 #frequency of operation in Hz\n", + "a=4*10**-2 #in m\n", + "b=2*10**-2 #in m\n", + "u=3*10**8 #velocity in m/s\n", + "Pavg=2*10**-3 #average power in W\n", + "\n", + "#Calculations\n", + "\n", + "fc=u/(2*a) #cutoff frequency in Hz\n", + "n=377/scipy.sqrt(1-(fc/f)**2) #intrinsic wave impedance in ohms\n", + "E=scipy.sqrt(4*n*Pavg/(a*b)) #peak value of electric field in V/m\n", + "\n", + "#Result\n", + "\n", + "print 'Peak value of electric field =',round(E,2),'V/m'" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "Peak value of electric field = 63.77 V/m\n" + ] + } + ], + "prompt_number": 4 + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "<h3>Example 12.6, Page number: 571<h3>" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + " \n", + "\n", + "import scipy\n", + "\n", + "#Variable declaration\n", + "\n", + "cc=5.8*10**7 #in S/m\n", + "f=4.8*10**9 #in Hz\n", + "c=10**-17 #in S/m\n", + "Uo=4*scipy.pi*10**-7 #permeability of free space\n", + "Eo=10**-9/(36*scipy.pi) #permittivity of free space\n", + "Er=2.55 #relative permittivity\n", + "z=60*10**-2 #in m\n", + "l=4.2*10**-2 #in m\n", + "b=2.6*10**-2 #in m\n", + "P=1.2*10**3 #in W\n", + "\n", + "#Calculations\n", + "\n", + "n=377/scipy.sqrt(Er)\n", + "u=3*10**8/scipy.sqrt(Er)\n", + "fc=u/(2*l)\n", + "ad=c*n/(2*scipy.sqrt(1-(fc/f)**2))\n", + "Rs=scipy.sqrt(scipy.pi*f*Uo/cc)\n", + "ac=2*Rs*(0.5+(b/l)*(fc/f)**2)/(b*n*scipy.sqrt(1-(fc/f)**2))\n", + "a=ac\n", + "Pd=P*(scipy.e**(2*a*z)-1)\n", + "\n", + "#Result\n", + "\n", + "print 'power dissipated =',round(Pd,3),'W'\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "power dissipated = 6.096 W\n" + ] + } + ], + "prompt_number": 5 + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "<h3>Example 12.8, Page number: 579<h3>" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + " \n", + "\n", + "import scipy\n", + "\n", + "#Variable Declaration\n", + " \n", + "a=5*10**-2 #in m\n", + "b=4*10**-2 #in m\n", + "c=10*10**-2 #in m\n", + "C=5.8*10**7 #in mhos/m\n", + "Uo=4*scipy.pi*10**-7 #permeability of free space\n", + "u=3*10**8 #speed of wave in m/s\n", + "\n", + "#Calculations\n", + "\n", + "def f(m,n,p):\n", + " fr=scipy.sqrt((m/a)**2+(n/b)**2+(p/c)**2)*u/2 #resonant frequency in Hz\n", + " print round(fr*10**-9,3)\n", + " \n", + "\n", + "f101=3.35*10**9\n", + "d=scipy.sqrt(1/(scipy.pi*f101*Uo*C))\n", + "Q=(a*a+c*c)*a*b*c/(d*(2*b*(a**3+c**3)+a*c*(a*a+c*c))) #quality factor\n", + "\n", + "#Results\n", + "\n", + "print 'Thus the five lowest order modes in ascending order are '\n", + "print 'TE101, frequency in GHz ='\n", + "f(1,0,1)\n", + "print 'TE011, frequency in GHz ='\n", + "f(0,1,1)\n", + "print 'TE102, frequency in GHz ='\n", + "f(1,0,2)\n", + "print 'TE110, frequency in GHz ='\n", + "f(1,1,0)\n", + "print 'TE111 or TM111, frequency in GHz ='\n", + "f(1,1,1)\n", + "print 'Quality factor =',round(Q,0)" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "Thus the five lowest order modes in ascending order are \n", + "TE101, frequency in GHz =\n", + "3.354\n", + "TE011, frequency in GHz =\n", + "4.039\n", + "TE102, frequency in GHz =\n", + "4.243\n", + "TE110, frequency in GHz =\n", + "4.802\n", + "TE111 or TM111, frequency in GHz =\n", + "5.031\n", + "Quality factor = 14358.0\n" + ] + } + ], + "prompt_number": 6 + } + ], + "metadata": {} + } + ] }
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