{ "metadata": { "name": "", "signature": "sha256:8165b8e5dad1d709dff36c0fb8461bb25ed06730a63d035a743672c074cb35cf" }, "nbformat": 3, "nbformat_minor": 0, "worksheets": [ { "cells": [ { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "Chapter07, Loop Antenna" ] }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example No. 7.10.1, page : 7-16" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import numpy as np\n", "A=1 #m\u00b2(Area of loop)\n", "N=400 #no. of turns\n", "Q=100 #Quality factor\n", "theta=60 #degree(angle)\n", "Erms=10 #\u00b5V/m(field strength)\n", "f=1 #MHz(tuned frequency)\n", "c=3*10**8 #m/s##Speed of light\n", "lamda=c/(f*10**6) #m(Wavelength)\n", "Vr=Q*2*np.pi*A*N*np.cos(theta*np.pi/180)*Erms*10**-6/lamda #V(reciever input voltage)\n", "print \"Input voltage to the receiver = %0.3f mV \" %(Vr*1000)" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Input voltage to the receiver = 4.189 mV \n" ] } ], "prompt_number": 3 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example No. 7.10.2, page : 7-17" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import numpy as np\n", "N=12 #no. of turns\n", "A=1 #m\u00b2(Area of loop)\n", "Erms=100 #\u00b5V/m(field strength)\n", "f=10 #MHz(tuned frequency)\n", "theta=0 #degree(angle)\n", "c=3*10**8 #m/s##Speed of light\n", "lamda=c/(f*10**6) #m(Wavelength)\n", "Vr=2*np.pi*A*N*np.cos(theta*np.pi/180)*Erms*10**-6/lamda #V(reciever input voltage)\n", "print \"Voltage induced in loop = %0.2f \u00b5V/m \" %(Vr*10**6) " ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Voltage induced in loop = 251.33 \u00b5V/m \n" ] } ], "prompt_number": 4 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example No. 7.10.3, page : 7-17" ] }, { "cell_type": "code", "collapsed": false, "input": [ "N=25 #no. of turns\n", "Vrms=150 #\u00b5V(emf induced)\n", "f=500 #kHz(tuned frequency)\n", "A=0.5**2 #m\u00b2(Area of loop)\n", "theta=0 #degree(angle)\n", "c=3*10**8 #m/s##Speed of light\n", "lamda=c/(f*10**3) #m(Wavelength)\n", "Erms=lamda/(2*np.pi*A*N*np.cos(theta*np.pi/180))*Vrms*10**-6 #V/m(maximum emf induced)\n", "print \"Field strength = %0.3f mV/m \"%(Erms*10**3) " ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Field strength = 2.292 mV/m \n" ] } ], "prompt_number": 7 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example No. 7.10.4, page : 7-17" ] }, { "cell_type": "code", "collapsed": false, "input": [ "N1=1.0 #no. of turns in primary\n", "N2=8.0 #no. of turns in secondary\n", "#a=lamda/25 \n", "aBYlamda=1.0/25 #(temporary calculation)\n", "#A=np.pi*a**2\n", "A_BY_lamda_sqr=np.pi*aBYlamda**2 #(temporary calculation)\n", "Rr1=31200*(N1*A_BY_lamda_sqr)**2 #\u03a9(Radiation resistance for single turn)\n", "print \"Radiation resistance for single turn loop = %0.4f \u03a9 \" %(Rr1) \n", "Rr2=31200*(N2*A_BY_lamda_sqr)**2 #\u03a9(Radiation resistance for 8 turn)\n", "print \"Radiation resistance for 8 turn loop = %0.2f \u03a9 \" %Rr2 " ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Radiation resistance for single turn loop = 0.7883 \u03a9 \n", "Radiation resistance for 8 turn loop = 50.45 \u03a9 \n" ] } ], "prompt_number": 11 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example No. 7.10.5, page : 7-18" ] }, { "cell_type": "code", "collapsed": false, "input": [ "from __future__ import division\n", "f=100 #MHz(Operating frequency)\n", "c=3*10**8 #m/s##Speed of light\n", "lamda=c/(f*10**6) #m(Wavelength)\n", "a=lamda/25 #m(radius)\n", "C=2*np.pi*a #m(Circumference)\n", "d=2*10**-4*lamda #m(Spacing)\n", "print \"For single turn : \" \n", "N=1 #n. of turns\n", "RL_BY_Rr=3430.0/(C**3*f**(3.5)*N*d) #(temporary calculation)\n", "K=1/(1+RL_BY_Rr)*100 #%(Radiation efficiency)\n", "print \"Radiation efficiency of single turn = %0.2f %%\" %K\n", "print \"For Eight turn : \" \n", "N=8 #no. of turns\n", "RL_BY_Rr=3430/(C**3*f**(3.5)*N*d) #(temporary calculation)\n", "K=1/(1+RL_BY_Rr)*100 #%(Radiation efficiency)\n", "print \"Radiation efficiency of eight turn = %0.2f %%\" % K" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "For single turn : \n", "Radiation efficiency of single turn = 42.85 %\n", "For Eight turn : \n", "Radiation efficiency of eight turn = 85.71 %\n" ] } ], "prompt_number": 14 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example No. 7.10.6, page : 7-19" ] }, { "cell_type": "code", "collapsed": false, "input": [ "from fractions import Fraction\n", "a=0.5 #m(radius)\n", "f=0.9 #MHz(OPerating frequency)\n", "c=3*10**8 #m/s##Speed of light\n", "lamda=c/(f*10**6) #m(wavelength)\n", "C=2*np.pi*a #m(Circumference)\n", "if C/lamda<1/3:\n", " D=3/2 #Directivity\n", "elif C/lamda>1/3:\n", " D=0.682*C/lamda #Directivity\n", "\n", "print \"Directivity :\" ,Fraction(D)" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Directivity : 3/2\n" ] } ], "prompt_number": 18 } ], "metadata": {} } ] }