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author | kinitrupti | 2015-10-15 17:40:30 +0530 |
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committer | kinitrupti | 2015-10-15 17:40:30 +0530 |
commit | 8e4f9ec414f553746330423a974684bbac2163a8 (patch) | |
tree | 7d91d4997a3962c3ad62355ad369f7b6b7738ddb /Power_Electronics_by_P_S_Bimbhra/Chapter13_4.ipynb | |
parent | 79c8f29f70cc014d5fd8b9900d3c19309134bc1d (diff) | |
download | Python-Textbook-Companions-8e4f9ec414f553746330423a974684bbac2163a8.tar.gz Python-Textbook-Companions-8e4f9ec414f553746330423a974684bbac2163a8.tar.bz2 Python-Textbook-Companions-8e4f9ec414f553746330423a974684bbac2163a8.zip |
solved errors
Diffstat (limited to 'Power_Electronics_by_P_S_Bimbhra/Chapter13_4.ipynb')
-rwxr-xr-x | Power_Electronics_by_P_S_Bimbhra/Chapter13_4.ipynb | 680 |
1 files changed, 339 insertions, 341 deletions
diff --git a/Power_Electronics_by_P_S_Bimbhra/Chapter13_4.ipynb b/Power_Electronics_by_P_S_Bimbhra/Chapter13_4.ipynb index 62d2a926..a5664090 100755 --- a/Power_Electronics_by_P_S_Bimbhra/Chapter13_4.ipynb +++ b/Power_Electronics_by_P_S_Bimbhra/Chapter13_4.ipynb @@ -1,342 +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",
- "reg2=(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": [
- {
- "ename": "NameError",
- "evalue": "name 'reg1' is not defined",
- "output_type": "pyerr",
- "traceback": [
- "\u001b[1;31m---------------------------------------------------------------------------\u001b[0m\n\u001b[1;31mNameError\u001b[0m Traceback (most recent call last)",
- "\u001b[1;32m<ipython-input-2-ffdbe43fd921>\u001b[0m in \u001b[0;36m<module>\u001b[1;34m()\u001b[0m\n\u001b[0;32m 25\u001b[0m \u001b[1;32mprint\u001b[0m\u001b[1;33m(\u001b[0m\u001b[1;34m\"for pf=1\"\u001b[0m\u001b[1;33m)\u001b[0m\u001b[1;33m\u001b[0m\u001b[0m\n\u001b[0;32m 26\u001b[0m \u001b[1;32mprint\u001b[0m\u001b[1;33m(\u001b[0m\u001b[1;34m\"load voltage=%.2f V\"\u001b[0m \u001b[1;33m%\u001b[0m\u001b[0mV_l1\u001b[0m\u001b[1;33m)\u001b[0m\u001b[1;33m\u001b[0m\u001b[0m\n\u001b[1;32m---> 27\u001b[1;33m \u001b[1;32mprint\u001b[0m\u001b[1;33m(\u001b[0m\u001b[1;34m\"voltage regulation=%.2f\"\u001b[0m \u001b[1;33m%\u001b[0m\u001b[0mreg1\u001b[0m\u001b[1;33m)\u001b[0m\u001b[1;33m\u001b[0m\u001b[0m\n\u001b[0m\u001b[0;32m 28\u001b[0m \u001b[1;32mprint\u001b[0m\u001b[1;33m(\u001b[0m\u001b[1;34m\"system utilisation factor=%.3f\"\u001b[0m \u001b[1;33m%\u001b[0m\u001b[0mutf1\u001b[0m\u001b[1;33m)\u001b[0m\u001b[1;33m\u001b[0m\u001b[0m\n\u001b[0;32m 29\u001b[0m \u001b[1;32mprint\u001b[0m\u001b[1;33m(\u001b[0m\u001b[1;34m\"energy consumed(in units)=%.1f\"\u001b[0m \u001b[1;33m%\u001b[0m\u001b[1;33m(\u001b[0m\u001b[0mP_l1\u001b[0m\u001b[1;33m/\u001b[0m\u001b[1;36m1000\u001b[0m\u001b[1;33m)\u001b[0m\u001b[1;33m)\u001b[0m\u001b[1;33m\u001b[0m\u001b[0m\n",
- "\u001b[1;31mNameError\u001b[0m: name 'reg1' is not defined"
- ]
- },
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "for pf=1\n",
- "load voltage=229.13 V\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": {}
- }
- ]
+{ + "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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