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| author | hardythe1 | 2014-07-25 13:33:31 +0530 |
|---|---|---|
| committer | hardythe1 | 2014-07-25 13:33:31 +0530 |
| commit | 1c1ea29e3e213559fef5f928df109b7d17c21f24 (patch) | |
| tree | a1d38eb039e19d9e84b6e769cec04d59e7179e66 /Electrical_Circuit_Theory_And_Technology/chapter_44-checkpoint_2.ipynb | |
| parent | efb9ead5d9758d5d0bed7a22069320b14f972e40 (diff) | |
| download | Python-Textbook-Companions-1c1ea29e3e213559fef5f928df109b7d17c21f24.tar.gz Python-Textbook-Companions-1c1ea29e3e213559fef5f928df109b7d17c21f24.tar.bz2 Python-Textbook-Companions-1c1ea29e3e213559fef5f928df109b7d17c21f24.zip | |
removing unwanted and adding book
Diffstat (limited to 'Electrical_Circuit_Theory_And_Technology/chapter_44-checkpoint_2.ipynb')
| -rwxr-xr-x | Electrical_Circuit_Theory_And_Technology/chapter_44-checkpoint_2.ipynb | 1093 |
1 files changed, 0 insertions, 1093 deletions
diff --git a/Electrical_Circuit_Theory_And_Technology/chapter_44-checkpoint_2.ipynb b/Electrical_Circuit_Theory_And_Technology/chapter_44-checkpoint_2.ipynb deleted file mode 100755 index 03d830a4..00000000 --- a/Electrical_Circuit_Theory_And_Technology/chapter_44-checkpoint_2.ipynb +++ /dev/null @@ -1,1093 +0,0 @@ -{
- "metadata": {
- "name": ""
- },
- "nbformat": 3,
- "nbformat_minor": 0,
- "worksheets": [
- {
- "cells": [
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h1>Chapter 44: Transmission lines</h1>"
- ]
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 1, page no. 873</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine (a) the wavelength on the line, and (b) the speed of transmission of a signal.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "f = 1910;# in Hz\n",
- "b = 0.05;# in rad/km\n",
- "\n",
- "#calculation:\n",
- "w = 2*math.pi*f\n",
- " #wavelength \n",
- "Y = 2*math.pi/b\n",
- " #speed of transmission\n",
- "u = f*Y\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n wavelength Y is \",round(Y,1),\" km\"\n",
- "print \"\\n speed of transmission \",round(u,1),\"km/sec\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " wavelength Y is 125.7 km\n",
- "\n",
- " speed of transmission 240017.7 km/sec"
- ]
- }
- ],
- "prompt_number": 1
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 2, page no. 873</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine, for a frequency of operation of 1 kHz, \n",
- "#(a) the phase delay, \n",
- "#(b) the wavelength on the line, and \n",
- "#(c) the velocity of propagation (in metres per second) of the signal.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "L = 0.004;# in Henry/loop\n",
- "C = 0.004E-6;# in F/loop\n",
- "f = 1000;# in Hz\n",
- "\n",
- " #calculation:\n",
- "w = 2*math.pi*f\n",
- " #phase delay\n",
- "b = w*(L*C)**0.5\n",
- " #wavelength \n",
- "Y = 2*math.pi/b\n",
- " #speed of transmission\n",
- "u = f*Y\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n phase delay is \",round(b,3),\" rad/km\"\n",
- "print \"\\n wavelength Y is \",Y,\" km\"\n",
- "print \"\\n speed of transmission \",u,\"km/sec\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " phase delay is 0.025 rad/km\n",
- "\n",
- " wavelength Y is 250.0 km\n",
- "\n",
- " speed of transmission 250000.0 km/sec"
- ]
- }
- ],
- "prompt_number": 2
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 3, page no. 874</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#determine the voltage at a point 10 km down the line,\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "a = 0.25;# in Np/km\n",
- "b = 0.20;# in rad/km\n",
- "Vs = 5;# in Volts\n",
- "n = 10;# in km\n",
- "f = 2000;# in Hz\n",
- "\n",
- " #calculation:\n",
- "w = 2*math.pi*f\n",
- " #the voltage 10 km down the line\n",
- "r = a + 1j*b\n",
- "VR = Vs*cmath.e**(-1*n*r)\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n Result \\n\\n\"\n",
- "print \"voltage 10 km down the line is \",round(abs(VR),2),\"/_\",round(cmath.phase(complex(VR.real,VR.imag))*180/math.pi,2),\"deg V\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- " Result \n",
- "\n",
- "\n",
- "voltage 10 km down the line is 0.41 /_ -114.59 deg V\n"
- ]
- }
- ],
- "prompt_number": 1
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 4, page no. 875</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine the magnitude and phase of the current at the receiving end,\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "a = 0.5;# in Np/km\n",
- "b = 0.25;# in rad/km\n",
- "rvs = 2;# in Volts\n",
- "thetavs = 0;# in degrees\n",
- "rzo = 800;# in ohm\n",
- "thetazo = -25;# in degrees\n",
- "n = 5;# in km\n",
- "\n",
- "#calculation:\n",
- " #voltage\n",
- "Vs = rvs*math.cos(thetavs*math.pi/180) + 1j*rvs*math.sin(thetavs*math.pi/180)\n",
- " #characteristic impedance\n",
- "Zo = rzo*math.cos(thetazo*math.pi/180) + 1j*rzo*math.sin(thetazo*math.pi/180)\n",
- " # receiving end voltage\n",
- "r = a + 1j*b\n",
- "VR = Vs*cmath.e**(-1*n*r)\n",
- " #Receiving end current,\n",
- "IR = VR/Zo\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"Receiving end current, IR is \",round(abs(IR)*1E3,3),\"/_\",round(cmath.phase(complex(IR.real,IR.imag))*180/math.pi,2),\"deg mA\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "Receiving end current, IR is 0.205 /_ -46.62 deg mA\n"
- ]
- }
- ],
- "prompt_number": 2
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 5, page no. 875</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine the output voltage if the length of the line is doubled.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "Vs = 8;# in Volts\n",
- "VR = 2;# in Volts\n",
- "x = 2; \n",
- "\n",
- "#calculation:\n",
- " # receiving end voltage VR = Vs*e**(-nr)\n",
- " #e**-nr = p\n",
- "p = VR/Vs\n",
- " #If the line is doubled in length, then\n",
- "VR = Vs*(p)**2\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n Receiving end voltage If the line is doubled in length, VR is \",abs(VR),\" V\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " Receiving end voltage If the line is doubled in length, VR is 0.5 V"
- ]
- }
- ],
- "prompt_number": 5
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 6, page no. 876</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine the characteristic impedance of the line at this frequency.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "rzoc = 800;# in ohm\n",
- "thetazoc = -50;# in degrees\n",
- "rzsc = 413;# in ohm\n",
- "thetazsc = -20;# in degrees\n",
- "f = 1500;# in Hz\n",
- "\n",
- " #calculation:\n",
- " #open circuit impedance\n",
- "Zoc = rzoc*math.cos(thetazoc*math.pi/180) + 1j*rzoc*math.sin(thetazoc*math.pi/180)\n",
- " #short circuit impedance\n",
- "Zsc = rzsc*math.cos(thetazsc*math.pi/180) + 1j*rzsc*math.sin(thetazsc*math.pi/180)\n",
- " #characteristic impedance Zo\n",
- "Zo = (Zoc*Zsc)**0.5\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"characteristic impedance Zo is\",round(abs(Zo)),\"/_\",round(cmath.phase(complex(Zo.real,Zo.imag))*180/math.pi,2),\"deg ohm\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "characteristic impedance Zo is 575.0 /_ -35.0 deg ohm\n"
- ]
- }
- ],
- "prompt_number": 3
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 7, page no. 877</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine the characteristic impedance of the line when the frequency is 2 kHz.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "R = 15;# in ohm/loop km\n",
- "L = 0.0034;# in H/loop km\n",
- "C = 10E-9;# in F/km\n",
- "G = 3E-6;# in S/km\n",
- "f = 2000;# in Hz\n",
- "\n",
- " #calculation:\n",
- "w = 2*math.pi*f\n",
- " #characteristic impedance Zo\n",
- "Zo = ((R + 1j*w*L)/(G + 1j*w*C))**0.5\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"characteristic impedance Zo is \",round(abs(Zo),0),\"/_\",round(cmath.phase(complex(Zo.real,Zo.imag))*180/math.pi,2),\"deg ohm\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "characteristic impedance Zo is 600.0 /_ -8.99 deg ohm\n"
- ]
- }
- ],
- "prompt_number": 4
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 8, page no. 879</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine, at an operating frequency of 400 kHz, (a) the characteristic impedance,\n",
- "#(b) the propagation coefficient, (c) the wavelength on the line, and \n",
- "#(d) the velocity of propagation, in metres per second, of a signal.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "L = 0.0005;# in H/loop km\n",
- "C = 0.12E-6;# in F/km\n",
- "f = 400000;# in Hz\n",
- "\n",
- "#calculation:\n",
- "w = 2*math.pi*f\n",
- " #characteristic impedance Zo\n",
- "Zo = (L/C)**0.5\n",
- " #the propagation coefficient\n",
- "r = 1j*w*(L*C)**0.5\n",
- " #the attenuation coefficient \n",
- "a = r.real\n",
- " #the phaseshift coefficient\n",
- "b = r.imag\n",
- " #wavelength\n",
- "Y = 2*math.pi/b\n",
- " #velocity of propagation \n",
- "u = f*Y\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n characteristic impedance Zo is \",abs(Zo),\"ohm\"\n",
- "print \"\\n propagation coefficient is \",a,\" +(\",round(b,2),\")i\"\n",
- "print \"\\n wavelength Y is \",round(Y*1E3,0),\"m\"\n",
- "print \"\\n speed of transmission \",round(u,2),\"km/sec\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " characteristic impedance Zo is 64.5497224368 ohm\n",
- "\n",
- " propagation coefficient is 0.0 +( 19.47 )i\n",
- "\n",
- " wavelength Y is 323.0 m\n",
- "\n",
- " speed of transmission 129099.44 km/sec"
- ]
- }
- ],
- "prompt_number": 8
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 9, page no. 880</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine for the line (a) the characteristic impedance,\n",
- "#(b) the propagation coefficient, (c) the attenuation coefficient and\n",
- "#(d) the phase-shift coefficient\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "R = 25;# in ohm/loop km\n",
- "L = 0.005;# in H/loop km\n",
- "C = 0.04E-6;# in F/km\n",
- "G = 80E-6;# in S/km\n",
- "f = 1000;# in Hz\n",
- "\n",
- " #calculation:\n",
- "w = 2*math.pi*f\n",
- " #characteristic impedance Zo\n",
- "Zo = ((R + 1j*w*L)/(G + 1j*w*C))**0.5\n",
- " #the propagation coefficient\n",
- "r = ((R + 1j*w*L)*(G + 1j*w*C))**0.5\n",
- " #the attenuation coefficient \n",
- "a = r.real\n",
- " #the phaseshift coefficient\n",
- "b = r.imag\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"characteristic impedance Zo is\",round(abs(Zo),2),\"/_\",round(cmath.phase(complex(Zo.real,Zo.imag))*180/math.pi,2),\"deg ohm\"\n",
- "print \"\\n propagation coefficient is \",round(abs(r),4),\"/_\",round(cmath.phase(complex(a,b))*180/math.pi,2),\"deg\"\n",
- "print \"\\n attenuation coefficient is \",round(a,4),\" Np/km\"\n",
- "print \"\\n the phase-shift coefficient \",round(b,4),\" rad/km\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "characteristic impedance Zo is 390.16 /_ -10.43 deg ohm\n",
- "\n",
- " propagation coefficient is 0.1029 /_ 61.92 deg\n",
- "\n",
- " attenuation coefficient is 0.0484 Np/km\n",
- "\n",
- " the phase-shift coefficient 0.0908 rad/km\n"
- ]
- }
- ],
- "prompt_number": 5
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 10, page no. 881</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#determine (a) the characteristic impedance, \n",
- "#(b) the propagation coefficient, \n",
- "#(c) the attenuation and phase-shift coefficients, \n",
- "#(d) the sending-end current, \n",
- "#(e) the receiving-end current, \n",
- "#(f) the wavelength on the line, and \n",
- "#(g) the speed of transmission of signal.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "R = 8;# in ohm/loop km\n",
- "L = 0.003;# in H/loop km\n",
- "C = 7500E-12;# in F/km\n",
- "G = 0.25E-6;# in S/km\n",
- "f = 1000;# in Hz\n",
- "n = 300;# in km\n",
- "Zg = 400 + 1j*0;# in ohm\n",
- "Vg = 10;# in Volts\n",
- "\n",
- " #calculation:\n",
- "w = 2*math.pi*f\n",
- " #characteristic impedance Zo\n",
- "Zo = ((R + 1j*w*L)/(G + 1j*w*C))**0.5\n",
- " #the propagation coefficient\n",
- "r = ((R + 1j*w*L)*(G + 1j*w*C))**0.5\n",
- " #the attenuation coefficient \n",
- "a = r.real\n",
- " #the phaseshift coefficient\n",
- "b = r.imag\n",
- " #the sending-end current,\n",
- "Is = Vg/(Zg + Zo)\n",
- " #the receiving-end current,\n",
- "IR = Is*cmath.e**(-1*n*r)\n",
- " #wavelength\n",
- "Y = 2*math.pi/b\n",
- " #velocity of propagation \n",
- "u = f*Y\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"characteristic impedance Zo is\",round(abs(Zo),1),\"/_\",round(cmath.phase(complex(Zo.real,Zo.imag))*180/math.pi,2),\"deg ohm\"\n",
- "print \"propagation coefficient is \",round(abs(r),5),\"/_\",round(cmath.phase(complex(r.real,r.imag))*180/math.pi,2),\"deg\"\n",
- "print \"attenuation coefficient is \",round(a,5),\" Np/km and the phaseshift coefficient \",round(b,5),\" rad/km\"\n",
- "print \"sending-end current Is is \",round(abs(Is)*1E3,3),\"/_\",round(cmath.phase(complex(Is.real,Is.imag))*180/math.pi,2),\"deg mA\"\n",
- "print \"receiving-end current IR is\",round(abs(IR)*1E3,3),\"/_\",round(cmath.phase(complex(IR.real,IR.imag))*180/math.pi,2),\"deg mA\"\n",
- "print \"wavelength Y is \",round(Y,1),\" km\"\n",
- "print \"speed of transmission \",round(u,1),\"km/sec\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "characteristic impedance Zo is 659.2 /_ -11.35 deg ohm\n",
- "propagation coefficient is 0.03106 /_ 78.35 deg\n",
- "attenuation coefficient is 0.00627 Np/km and the phaseshift coefficient 0.03042 rad/km\n",
- "sending-end current Is is 9.485 /_ 7.07 deg mA\n",
- "receiving-end current IR is 1.445 /_ -155.88 deg mA\n",
- "wavelength Y is 206.5 km\n",
- "speed of transmission 206521.1 km/sec\n"
- ]
- }
- ],
- "prompt_number": 6
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 11, page no. 884</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine by how much the inductance should be increased to satisfy the condition for minimum distortion.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "R = 10;# in ohm/loop km\n",
- "L = 0.0015;# in H/loop km\n",
- "C = 0.06E-6;# in F/km\n",
- "G = 1.2E-6;# in S/km\n",
- "\n",
- " #calculation:\n",
- " #the condition for minimum distortion is given by LG = CR, from which,\n",
- "Lm = C*R/G\n",
- "dL = Lm - L\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n inductance should be increased by \",round(dL*1E3,1),\"mH/loop km for minimum distortion\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " inductance should be increased by 498.5 mH/loop km for minimum distortion"
- ]
- }
- ],
- "prompt_number": 11
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 12, page no. 884</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine, for minimum distortion at a frequency of 1.5 kHz \n",
- "#(a) the value of inductance per loop kilometre required, \n",
- "#(b) the propagation coefficient, \n",
- "#(c) the velocity of propagation of signal, and \n",
- "#(d) the wavelength on the line\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "R = 80;# in ohm/loop km\n",
- "C = 5E-9;# in F/km\n",
- "G = 2E-6;# in S/km\n",
- "f = 1500;# in Hz\n",
- "\n",
- " #calculation:\n",
- "w = 2*math.pi*f\n",
- " #the condition for minimum distortion is given by LG = CR, from which, inductance\n",
- "L = C*R/G\n",
- " #attenuation coefficient,\n",
- "a = (R*G)**0.5\n",
- " #phase shift coefficient,\n",
- "b = w*(L*C)**0.5\n",
- " #propagation coefficient,\n",
- "r = a + 1j*b\n",
- " #velocity of propagation,\n",
- "u = 1/(L*C)**0.5\n",
- " #wavelength\n",
- "Y = u/f\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n inductance is \",round(L,2),\" H\"\n",
- "print \"\\n propagation coefficient is \",round(a,2),\" +(\",round(b,2),\")i\"\n",
- "print \"\\n speed of transmission \",round(u,2),\"km/sec\"\n",
- "print \"\\n wavelength Y is \",round(Y,2),\" km\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " inductance is 0.2 H\n",
- "\n",
- " propagation coefficient is 0.01 +( 0.3 )i\n",
- "\n",
- " speed of transmission 31622.78 km/sec\n",
- "\n",
- " wavelength Y is 21.08 km\n"
- ]
- }
- ],
- "prompt_number": 7
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 13, page no. 888</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#calculate the value of (a) the reflection coefficient for the line, (b) the incident current, \n",
- "#(c) the incident voltage, (d) the reflected current, and (e) the reflected voltage \n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "Zo = 75;# in ohm\n",
- "ZR = 250;# in ohm\n",
- "VR = 10;# in Volts\n",
- "\n",
- "#calculation:\n",
- " #reflection coefficient\n",
- "p = (Zo - ZR)/(Zo + ZR)\n",
- " #Current flowing in the terminating load\n",
- "IR = VR/ZR\n",
- " #incident current, Ii\n",
- "Ii = IR/(1 + p)\n",
- " #incident voltage, Vi \n",
- "Vi = Ii*Zo\n",
- " #reflected current, Ir\n",
- "Ir = IR - Ii\n",
- " #reflected voltage, Vr\n",
- "Vr = -1*Ir*Zo\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n reflection coefficient is \",round(p,3),\"\"\n",
- "print \"\\n incident current, Ii is \",round(Ii,4),\" A\"\n",
- "print \"\\n incident voltage, Vi is \",round(Vi,2),\" V\"\n",
- "print \"\\n reflected current, Ir is \",round(Ir,4),\" A\"\n",
- "print \"\\n reflected voltage, Vr is \",round(Vr,2),\" V\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " reflection coefficient is -0.538 \n",
- "\n",
- " incident current, Ii is 0.0867 A\n",
- "\n",
- " incident voltage, Vi is 6.5 V\n",
- "\n",
- " reflected current, Ir is -0.0467 A\n",
- "\n",
- " reflected voltage, Vr is 3.5 V"
- ]
- }
- ],
- "prompt_number": 13
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 14, page no. 889</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine the magnitude of the reflection coefficient in each case.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "Zo = 500 - 1j*40;# in ohm\n",
- "ZR1 = 500 + 1j*40;# in ohm\n",
- "ZR2 = 600 + 1j*0;# in ohm\n",
- "\n",
- " #calculation:\n",
- " #reflection coefficient\n",
- "p1 = (Zo - ZR1)/(Zo + ZR1)\n",
- "p2 = (Zo - ZR2)/(Zo + ZR2)\n",
- "p1mag = abs(p1)\n",
- "p2mag = abs(p2)\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n reflection coefficient (a)\",p1mag,\" and (b)\", round(p2mag,2),\"\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " reflection coefficient (a) 0.08 and (b) 0.1 "
- ]
- }
- ],
- "prompt_number": 14
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 15, page no. 890</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Determine (a) the magnitude of the ratio of the reflected to the incident voltage wave, and \n",
- "#(b) the incident voltage\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "rzo = 500;# in ohm\n",
- "thetazo = 0;# in degrees\n",
- "ZR = 320 + 1j*240;# in ohm\n",
- "rvr = 20;# in volts\n",
- "thetavr = 35;# in degrees\n",
- "\n",
- " #calculation:\n",
- " #voltage\n",
- "VR = rvr*math.cos(thetavr*math.pi/180) + 1j*rvr*math.sin(thetavr*math.pi/180)\n",
- " #characteristic impedance\n",
- "Zo = rzo*math.cos(thetazo*math.pi/180) + 1j*rzo*math.sin(thetazo*math.pi/180)\n",
- " #the ratio of the reflected to the incident voltage \n",
- " #vr = VR/Vi\n",
- "vr = (ZR - Zo)/(Zo + ZR)\n",
- "vrmag = abs(vr)\n",
- " #incident voltage, Vi\n",
- "Vi = VR/vr\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n the magnitude of the ratio Vr : Vi is \",round(vrmag,3),\"\"\n",
- "print \"\\n incident voltage, Vi is \",round(abs(Vi),1),\"/_\",round(cmath.phase(complex(Vi.real,Vi.imag))*180/math.pi,2),\"deg V\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " the magnitude of the ratio Vr : Vi is 0.351 \n",
- "\n",
- " incident voltage, Vi is 57.0 /_ -75.56 deg V\n"
- ]
- }
- ],
- "prompt_number": 8
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 16, page no. 895</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#determine (a) the reflection coefficient and (b) the standing-wave ratio.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "rzo = 600;# in ohm\n",
- "thetazo = 0;# in degrees\n",
- "ZR = 400 + 250j;# in ohm\n",
- "\n",
- " #calculation:\n",
- " #characteristic impedance\n",
- "Zo = rzo*math.cos(thetazo*math.pi/180) + 1j*rzo*math.sin(thetazo*math.pi/180)\n",
- " #reflection coefficient\n",
- "p = (Zo - ZR)/(Zo + ZR)\n",
- "pmag = abs(p)\n",
- " #standing-wave ratio,\n",
- "s = (1 + pmag)/(1 - pmag)\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n reflection coefficient, is \",round(abs(p),4),\"/_\",round(cmath.phase(complex(p.real,p.imag))*180/math.pi,2),\"deg\"\n",
- "print \"\\n standing-wave ratio, s is \",round(s,3),\"\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " reflection coefficient, is 0.3106 /_ -65.38 deg\n",
- "\n",
- " standing-wave ratio, s is 1.901 "
- ]
- }
- ],
- "prompt_number": 16
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 17, page no. 896</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#Calculate (a) the standing-wave ratio, \n",
- "#(b) the load impedance, and\n",
- "#(c) the incident current flowing if the reflected current is 10 mA.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "rp = 0.2; \n",
- "thetap = -120;# in degrees\n",
- "Zo = 80;# in ohm\n",
- "Ir = 0.01;# in Amperes\n",
- "\n",
- "#calculation:\n",
- " #reflection coefficient\n",
- "p = rp*math.cos(thetap*math.pi/180) + 1j*rp*math.sin(thetap*math.pi/180)\n",
- " #standing-wave ratio,\n",
- "s = (1 + rp)/(1 - rp)\n",
- " #load impedance ZR \n",
- "ZR = Zo*(1 - p)/(1 + p)\n",
- " #incident current\n",
- "Ii = Ir*(s + 1)/(s - 1)\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n standing-wave ratio, s is \",s,\"\"\n",
- "print \"\\n load impedance ZR is \",round(ZR.real,2),\" +(\",round(ZR.imag,1),\")i ohm\"\n",
- "print \"\\n incident current is \",Ii,\" A\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " standing-wave ratio, s is 1.5 \n",
- "\n",
- " load impedance ZR is 91.43 +( 33.0 )i ohm\n",
- "\n",
- " incident current is 0.05 A\n"
- ]
- }
- ],
- "prompt_number": 9
- },
- {
- "cell_type": "markdown",
- "metadata": {},
- "source": [
- "<h3>Example 18, page no. 897</h3>"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "#determine the value of the reflected power.\n",
- "from __future__ import division\n",
- "import math\n",
- "import cmath\n",
- "#initializing the variables:\n",
- "s = 1.6;\n",
- "Pi = 0.2;# in Watts\n",
- "\n",
- "#calculation:\n",
- " #reflected power, Pr\n",
- "Pr = Pi*((s - 1)/(s + 1))**2\n",
- "\n",
- "\n",
- "#Results\n",
- "print \"\\n\\n Result \\n\\n\"\n",
- "print \"\\n reflected power, Pr is \",round(Pr*1E3,2),\" mW\""
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "\n",
- "\n",
- " Result \n",
- "\n",
- "\n",
- "\n",
- " reflected power, Pr is 10.65 mW"
- ]
- }
- ],
- "prompt_number": 18
- }
- ],
- "metadata": {}
- }
- ]
-}
\ No newline at end of file |