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author | kinitrupti | 2017-05-12 18:53:46 +0530 |
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committer | kinitrupti | 2017-05-12 18:53:46 +0530 |
commit | f270f72badd9c61d48f290c3396004802841b9df (patch) | |
tree | bc8ba99d85644c62716ce397fe60177095b303db /Power_Electronics_by_P.S._Bimbhra/Chapter13_4.ipynb | |
parent | 64d949698432e05f2a372d9edc859c5b9df1f438 (diff) | |
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diff --git a/Power_Electronics_by_P.S._Bimbhra/Chapter13_4.ipynb b/Power_Electronics_by_P.S._Bimbhra/Chapter13_4.ipynb new file mode 100755 index 00000000..a5664090 --- /dev/null +++ b/Power_Electronics_by_P.S._Bimbhra/Chapter13_4.ipynb @@ -0,0 +1,340 @@ +{ + "metadata": { + "name": "" + }, + "nbformat": 3, + "nbformat_minor": 0, + "worksheets": [ + { + "cells": [ + { + "cell_type": "heading", + "level": 1, + "metadata": {}, + "source": [ + "Chapter 13 : Power Factor Improvement" + ] + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 13.1, Page No 754" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "#initialisation of variables\n", + "V_s=250.0\n", + "R_l=5.0\n", + "I_l=20.0\n", + "V_l1=math.sqrt(V_s**2-(R_l*I_l)**2)\n", + "reg1=(V_s-V_l1)/V_s*100 \n", + "pf1=1.0\n", + "\n", + "#Calculations\n", + "P_l1=V_l1*I_l*pf1 #load power\n", + "P_r1=V_s*I_l*pf1 #max powwible system rating\n", + "utf1=P_l1*100/P_r1 \n", + "pf2=0.5\n", + " #(.5*V_l)**2+(.866*V_l+R_l*I_l)**2=V_s**2\n", + " #after solving\n", + "V_l2=158.35 \n", + "reg2=(V_s-V_l2)/V_s*100 \n", + "P_l2=V_l2*I_l*pf2 #load power\n", + "P_r2=V_s*I_l #max powwible system rating\n", + "utf2=P_l2*100/P_r2 \n", + "\n", + "\n", + "#Results\n", + "print(\"for pf=1\")\n", + "print(\"load voltage=%.2f V\" %V_l1)\n", + "print(\"voltage regulation=%.2f\" %reg1)\n", + "print(\"system utilisation factor=%.3f\" %utf1)\n", + "print(\"energy consumed(in units)=%.1f\" %(P_l1/1000))\n", + "print(\"for pf=.5\")\n", + "print(\"load voltage=%.2f V\" %V_l2)\n", + "print(\"voltage regulation=%.2f\" %reg2)\n", + "print(\"system utilisation factor=%.3f\" %utf2)\n", + "print(\"energy consumed(in units)=%.2f\" %(P_l2/1000))\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "for pf=1\n", + "load voltage=229.13 V\n", + "voltage regulation=8.35\n", + "system utilisation factor=91.652\n", + "energy consumed(in units)=4.6\n", + "for pf=.5\n", + "load voltage=158.35 V\n", + "voltage regulation=36.66\n", + "system utilisation factor=31.670\n", + "energy consumed(in units)=1.58\n" + ] + } + ], + "prompt_number": 2 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 13.2, Page No 756" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "#initialisation of variables\n", + "f=50.0\n", + "V_s=230.0\n", + "I_m1=2\n", + "pf1=.3\n", + "\n", + "#Calculations\n", + "I_c1=I_m1*math.sin(math.radians(math.degrees(math.acos(pf1))))\n", + "C1=I_c1/(2*math.pi*f*V_s) \n", + "I_m2=5\n", + "pf2=.5\n", + "I_c2=I_m2*math.sin(math.radians(math.degrees(math.acos(pf2))))\n", + "C2=I_c2/(2*math.pi*f*V_s) \n", + "I_m3=10\n", + "pf3=.7\n", + "I_c3=I_m3*math.sin(math.radians(math.degrees(math.acos(pf3))))\n", + "C3=I_c3/(2*math.pi*f*V_s) \n", + "\n", + "#Results\n", + "print(\"at no load\")\n", + "print(\"value of capacitance=%.3f uF\" %(C1*10**6))\n", + "print(\"at half full load\")\n", + "print(\"value of capacitance=%.3f uF\" %(C2*10**6))\n", + "print(\"at full load\")\n", + "print(\"value of capacitance=%.3f uF\" %(C3*10**6))" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "at no load\n", + "value of capacitance=26.404 uF\n", + "at half full load\n", + "value of capacitance=59.927 uF\n", + "at full load\n", + "value of capacitance=98.834 uF\n" + ] + } + ], + "prompt_number": 3 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 13.3 Page No 764" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "#initialisation of variables\n", + "I_c=10.0\n", + "f=50.0\n", + "V_s=230.0\n", + "\n", + "#Calculations\n", + "C=I_c/(2*math.pi*f*V_s) \n", + "I_l=10\n", + "L=V_s/(2*math.pi*f*I_l) \n", + "\n", + "#Results\n", + "print(\"value of capacitance=%.3f uF\" %(C*10**6))\n", + "print(\"value of inductor=%.3f mH\" %(L*1000))\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "value of capacitance=138.396 uF\n", + "value of inductor=73.211 mH\n" + ] + } + ], + "prompt_number": 4 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 13.4, Page No 765" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "#initialisation of variables\n", + "V_s=230.0\n", + "I_L=10.0\n", + "X_L=V_s/I_L\n", + "I_f1=6.0\n", + " #B=2*a-math.sin(2*a)\n", + "B=2*math.pi-I_f1*math.pi*X_L/V_s\n", + "a=0\n", + "i=1.0\n", + "for a in range(1,360):\n", + " b=2*a*math.pi/180-math.sin(math.radians(2*a)) \n", + " if math.fabs(B-b)<=0.001 : #by hit and trial\n", + " i=2\n", + " break\n", + "print(\"firing angle of TCR = %.1f deg\" %a)\n", + " #(a-.01)*180/math.pi)\n", + " \n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "firing angle of TCR = 359.0 deg\n" + ] + } + ], + "prompt_number": 5 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 13.5 Page No 766" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "#initialisation of variables\n", + "L=.01\n", + "\n", + "\n", + "#Calculations\n", + "print(\"for firing angle=90deg\")\n", + "a=90*math.pi/180\n", + "L_eff=math.pi*L/(2*math.pi-2*a+math.sin(2*a)) \n", + "print(\"effective inductance=%.0f mH\" %(L_eff*1000))\n", + "print(\"for firing angle=120deg\")\n", + "a=120*math.pi/180\n", + "L_eff=math.pi*L/(2*math.pi-2*a+math.sin(2*a)) \n", + "print(\"effective inductance=%.3f mH\" %(L_eff*1000))\n", + "print(\"for firing angle=150deg\")\n", + "a=150*math.pi/180\n", + "L_eff=math.pi*L/(2*math.pi-2*a+math.sin(2*a)) \n", + "print(\"effective inductance=%.2f mH\" %(L_eff*1000))\n", + "print(\"for firing angle=170deg\")\n", + "a=170*math.pi/180\n", + "L_eff=math.pi*L/(2*math.pi-2*a+math.sin(2*a)) \n", + "print(\"effective inductance=%.3f H\" %L_eff)\n", + "print(\"for firing angle=175deg\")\n", + "a=175*math.pi/180\n", + "L_eff=math.pi*L/(2*math.pi-2*a+math.sin(2*a)) \n", + "\n", + "#Results\n", + "print(\"effective inductance=%.2f H\" %L_eff)\n", + "print(\"for firing angle=180deg\")\n", + "a=180*math.pi/180\n", + "L_eff=math.pi*L/(2*math.pi-2*a+math.sin(2*a)) \n", + "print(\"effective inductance=%.3f H\" %L_eff)\n", + " #random value at firing angle =180 is equivalent to infinity as in answer in book\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "for firing angle=90deg\n", + "effective inductance=10 mH\n", + "for firing angle=120deg\n", + "effective inductance=25.575 mH\n", + "for firing angle=150deg\n", + "effective inductance=173.40 mH\n", + "for firing angle=170deg\n", + "effective inductance=4.459 H\n", + "for firing angle=175deg\n", + "effective inductance=35.51 H\n", + "for firing angle=180deg\n", + "effective inductance=-128265253940037.750 H\n" + ] + } + ], + "prompt_number": 6 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 13.6 Page No 766" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "import math\n", + "#initialisation of variables\n", + "Q=100.0*10**3\n", + "V_s=11.0*10**3\n", + "\n", + "#Calculations\n", + "f=50.0\n", + "L=V_s**2/(2*math.pi*f*Q) \n", + "\n", + "#Results\n", + "print(\"effective inductance=%.4f H\" %L)" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "effective inductance=3.8515 H\n" + ] + } + ], + "prompt_number": 7 + } + ], + "metadata": {} + } + ] +}
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