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| author | kinitrupti | 2017-05-12 18:40:35 +0530 |
|---|---|---|
| committer | kinitrupti | 2017-05-12 18:40:35 +0530 |
| commit | d36fc3b8f88cc3108ffff6151e376b619b9abb01 (patch) | |
| tree | 9806b0d68a708d2cfc4efc8ae3751423c56b7721 /Electric_Machines_by_Nagrath_&_Kothari/Chapter05_1.ipynb | |
| parent | 1b1bb67e9ea912be5c8591523c8b328766e3680f (diff) | |
| download | Python-Textbook-Companions-d36fc3b8f88cc3108ffff6151e376b619b9abb01.tar.gz Python-Textbook-Companions-d36fc3b8f88cc3108ffff6151e376b619b9abb01.tar.bz2 Python-Textbook-Companions-d36fc3b8f88cc3108ffff6151e376b619b9abb01.zip | |
Revised list of TBCs
Diffstat (limited to 'Electric_Machines_by_Nagrath_&_Kothari/Chapter05_1.ipynb')
| -rwxr-xr-x | Electric_Machines_by_Nagrath_&_Kothari/Chapter05_1.ipynb | 890 |
1 files changed, 0 insertions, 890 deletions
diff --git a/Electric_Machines_by_Nagrath_&_Kothari/Chapter05_1.ipynb b/Electric_Machines_by_Nagrath_&_Kothari/Chapter05_1.ipynb deleted file mode 100755 index 3103dd33..00000000 --- a/Electric_Machines_by_Nagrath_&_Kothari/Chapter05_1.ipynb +++ /dev/null @@ -1,890 +0,0 @@ -{
- "metadata": {
- "name": ""
- },
- "nbformat": 3,
- "nbformat_minor": 0,
- "worksheets": [
- {
- "cells": [
- {
- "cell_type": "heading",
- "level": 1,
- "metadata": {},
- "source": [
- "Chapter 05 : Basic concepts in rotating machines"
- ]
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.1, Page No 148"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# To calculate harmanic factor for stator\n",
- "\n",
- "S=36.0 #no of slots\n",
- "q=3.0 #no of phases\n",
- "p=4.0 #no of poles\n",
- "m=S/(q*p) #slots/pole/phase\n",
- "g=180*p/S #gamma elec\n",
- "\n",
- "#Calculations\n",
- "def bfctr(n):\n",
- " k=math.sin(math.radians(m*n*g/2))/(m*math.sin(math.radians(n*g/2))) \n",
- " return k\n",
- "\n",
- "K_b=bfctr(1) \n",
- "print(K_b,'K_b(fundamental)') \n",
- "\n",
- "K_b=bfctr(3.0) \n",
- "\n",
- "#Results\n",
- "print(K_b,'K_b(third harmonic)') \n",
- "\n",
- "K_b=bfctr(5.0) \n",
- "print(K_b,'K_b(fifth harmonic)') "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(0.9597950805239389, 'K_b(fundamental)')\n",
- "(0.6666666666666667, 'K_b(third harmonic)')\n",
- "(0.21756788155537973, 'K_b(fifth harmonic)')\n"
- ]
- }
- ],
- "prompt_number": 1
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.2, Page No 149"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# to find the frequency and phase and line voltages\n",
- "\n",
- "n=375.0 #speed in rpm\n",
- "p=16.0 #no of poles\n",
- "f=n*p/120.0 \n",
- "print(f,'freq(Hz)') \n",
- "S=144.0 #no of slots\n",
- "c=10.0 #no of conductors/slot\n",
- "\n",
- "#Calculations\n",
- "t=S*c/2 #no of turns\n",
- "ph=3 \n",
- "N_ph=t/ph #no of turns/ph\n",
- "g=180*p/S #slots angle\n",
- "m=S/(p*ph) #slots/pole/phase\n",
- "K_b=math.sin(math.radians(m*g/2.0))/(m*math.sin(math.radians(g/2))) #breadth factor\n",
- "phi=0.04 #flux per pole\n",
- "E_p=4.44*K_b*f*N_ph*phi \n",
- "\n",
- "#Results\n",
- "print(E_p,'phase voltage(V)') \n",
- "E_l=math.sqrt(3)*E_p \n",
- "print(E_l,'line voltage(V)') \n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(50.0, 'freq(Hz)')\n",
- "(2045.5152756126188, 'phase voltage(V)')\n",
- "(3542.936385019311, 'line voltage(V)')\n"
- ]
- }
- ],
- "prompt_number": 2
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.3, Page No 149"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# to find the phase and line voltages\n",
- "\n",
- "f=50 #freq\n",
- "n=600 #speed in rpm\n",
- "p=120*f/n \n",
- "ph=3 \n",
- "m=4 #slots/pole/ph\n",
- "S=p*ph*m #slots\n",
- "t=12 #turns per coil\n",
- "\n",
- "#Calculations\n",
- "N_ph=S*t/ph \n",
- "g=180*p/S \n",
- "K_b=math.sin(math.radians(m*g/2.0))/(m*math.sin(math.radians(g/2))) #breadth factor\n",
- "cp=10 #coil pitch\n",
- "pp=S/cp #pole pitch\n",
- "theta_sp=(pp-cp)*g #short pitch angle\n",
- "K_p=math.cos(math.radians(theta_sp/2))\n",
- "phi=.035 \n",
- "E_p=4.44*K_b*K_p*f*N_ph*phi\n",
- "\n",
- "#Results\n",
- "print(E_p,'phase voltage(V)') \n",
- "E_l=math.sqrt(3)*E_p \n",
- "print(E_l,'line voltage(V)')"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(3695.060690685099, 'phase voltage(V)')\n",
- "(6400.032853317139, 'line voltage(V)')\n"
- ]
- }
- ],
- "prompt_number": 3
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.4 Page No 150"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# to calculate flux/pole\n",
- "\n",
- "S=42 \n",
- "p=2 \n",
- "ph=3 \n",
- "m=S/(p*ph) #slots/pole/phase\n",
- "g=180*p/S #slots angle\n",
- "\n",
- "#Calculations\n",
- "K_b=math.sin(math.radians(m*g/2.0))/(m*math.sin(math.radians(g/2))) #breadth factor\n",
- "cp=17 \n",
- "pp=S/p \n",
- "theta_sp=(pp-cp)*g #short pitch angle\n",
- "K_p=math.cos(math.radians(theta_sp/2)) \n",
- "N_ph=S*2/(ph*p*2) #2 parallel paths\n",
- "E_p=2300/math.sqrt(3) \n",
- "phi=E_p/(4.44*K_b*K_p*f*N_ph) \n",
- "\n",
- "#Results\n",
- "print(phi,'flux/pole(Wb)') \n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(0.9245870891715325, 'flux/pole(Wb)')\n"
- ]
- }
- ],
- "prompt_number": 4
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.5, Page No 151"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# to calculate useful flux/pole and ares of pole shoe\n",
- "\n",
- "p=1500*1000.0 #power\n",
- "v=600.0 \n",
- "I_a=p/v \n",
- "cu=25*1000 #copper losses\n",
- "\n",
- "#Calculations\n",
- "R_a=cu/I_a**2 \n",
- "E_a=v+I_a*R_a \n",
- "n=200 \n",
- "Z=2500 \n",
- "p=16 \n",
- "A=16 \n",
- "phi=E_a*60*A/(p*n*Z) \n",
- "print(phi,'flux/pole(Wb)') \n",
- "fd=0.85 #flux density\n",
- "a=phi/fd \n",
- "\n",
- "#Results\n",
- "print(a,'area of pole shoe(m*m)') "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(0.0732, 'flux/pole(Wb)')\n",
- "(0.08611764705882353, 'area of pole shoe(m*m)')\n"
- ]
- }
- ],
- "prompt_number": 5
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.6, Page No 152"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# To calculate em power developed,mech power fed, torque provided by primemover\n",
- "\n",
- "phi=32*10**-3 #flux/pole\n",
- "n=1600 #speed in rpm\n",
- "Z=728 #no of conductors\n",
- "p=4 \n",
- "A=4 \n",
- "\n",
- "#Calculations\n",
- "E_a=phi*n*Z*(p/A)/60 \n",
- "I_a=100 \n",
- "P_e=E_a*I_a \n",
- "print(P_e,'electromagnetic power(W)') \n",
- "P_m=P_e \n",
- "print(P_m,'mechanical power(W) fed') \n",
- "w_m=2*math.pi*n/60 \n",
- "T=P_m/w_m \n",
- "\n",
- "#Results\n",
- "print(T,'primemover torque(Nm)') \n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(62122.66666666667, 'electromagnetic power(W)')\n",
- "(62122.66666666667, 'mechanical power(W) fed')\n",
- "(370.7673554268794, 'primemover torque(Nm)')\n"
- ]
- }
- ],
- "prompt_number": 6
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.9 Page No 163"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# To determine peak value of fundamental mmf\n",
- " \n",
- "f=50.0 \n",
- "n_s=300.0 \n",
- "p=120*f/n_s \n",
- "P=400*1000.0 #power\n",
- "V=3300.0 \n",
- "\n",
- "#Calculations\n",
- "I_L=P/(math.sqrt(3)*V) \n",
- "I_P=I_L \n",
- "I_m=math.sqrt(2)*I_P #max value of phase current\n",
- "S=180.0 \n",
- "g=180*p/S \n",
- "ph=3 \n",
- "m=S/(p*ph) #slots/pole/phase\n",
- "K_b=math.sin(math.radians(m*g/2.0))/(m*math.sin(math.radians(g/2))) #breadth factor\n",
- "c=8 #conductors/1 coil side\n",
- "N_ph=S*c/(ph*2) #turns/phase\n",
- "F_m=(4/math.pi)*K_b*(N_ph/p)*I_m \n",
- "F_peak=(3.0/2)*F_m \n",
- "\n",
- "#Results\n",
- "print(F_peak,'peak mmf(AT/pole)') \n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(2177.0157210889715, 'peak mmf(AT/pole)')\n"
- ]
- }
- ],
- "prompt_number": 7
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.10, Page No 164"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# (a)to calculate field current and flux/pole(b)to calculate open ckt ph and line voltages\n",
- "# (c)to caculate field current\n",
- "\n",
- "B_peak=1.65 \n",
- "g=.008 \n",
- "u_o=4*math.pi*10**-7 \n",
- "P=4 \n",
- "K_b=.957 \n",
- "N_field=364.0/2 \n",
- "\n",
- "#Calculations\n",
- "I_f=B_peak*math.pi*g*P/((4*u_o)*(K_b*N_field)) \n",
- "print(I_f,'field current(A)') \n",
- "l=1.02 #rotor length\n",
- "r=.41/2 #rotor radius\n",
- "phi=(4/P)*B_peak*l*r \n",
- "print(phi,'flux/pole(Wb)') \n",
- "N_ph=3*11*P/2 \n",
- "ga=60/3 #slot angle\n",
- "m=3 \n",
- "f=50 \n",
- "K_b=math.sin(math.radians(m*g/2.0))/(m*math.sin(math.radians(g/2))) #breadth factor\n",
- "E_ph=math.sqrt(2)*math.pi*K_b*f*N_ph*phi \n",
- "print(E_ph,'E_ph(V)') \n",
- "E_line=math.sqrt(3)*E_ph\n",
- "\n",
- "#Results\n",
- "print(E_line,'E_line(V)') \n",
- "I_fnew=.75*I_f \n",
- "print(I_fnew,'I_f(new)(A)') "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(189.46570670708599, 'field current(A)')\n",
- "(0.34501499999999996, 'flux/pole(Wb)')\n",
- "(5058.442114926427, 'E_ph(V)')\n",
- "(8761.478750198738, 'E_line(V)')\n",
- "(142.0992800303145, 'I_f(new)(A)')\n"
- ]
- }
- ],
- "prompt_number": 8
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.11 Page No 165"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# to find fundamental mmf wave,speed and its peak value\n",
- "\n",
- "p=4.0\n",
- "S=60.0 \n",
- "g=180*p/S \n",
- "ph=3 \n",
- "m=S/(p*ph) #slots/pole/phase\n",
- "\n",
- "#Calculations\n",
- "K_b=math.sin(math.radians(m*g/2.0))/(m*math.sin(math.radians(g/2))) #breadth factor\n",
- "I_L=48 \n",
- "I_P=I_L/math.sqrt(3) \n",
- "I_Pmax=I_P*math.sqrt(2) \n",
- "c=24 #conductors\n",
- "N_ph=S*c/(ph*2) #turns/phase\n",
- "F_m=(4/math.pi)*K_b*(N_ph/p)*I_Pmax \n",
- "print(F_m,'F_m(AT/pole)') \n",
- "F_peak=(3/2)*F_m \n",
- "\n",
- "#Results\n",
- "print(F_peak,'F_peak(AT/pole)') \n",
- "n=120*f/P \n",
- "print(n,'speed(rpm)') \n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(2864.325776100667, 'F_m(AT/pole)')\n",
- "(2864.325776100667, 'F_peak(AT/pole)')\n",
- "(1500, 'speed(rpm)')\n"
- ]
- }
- ],
- "prompt_number": 9
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.12 Page No 165"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# to calculate resultant air gap flux/pole\n",
- "\n",
- "F1=400.0 \n",
- "F2=850.0 \n",
- "a=123.6 \n",
- "\n",
- "#Calculations\n",
- "Fr=math.sqrt(F1**2+F2**2+2*F1*F2*math.cos(math.radians(a))) \n",
- "P=1.408*10**-4 #permeance/pole\n",
- "phi_r=P*Fr \n",
- "\n",
- "#Results\n",
- "print(phi_r,'air gap flux/pole(Wb)') "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(0.10017539016595711, 'air gap flux/pole(Wb)')\n"
- ]
- }
- ],
- "prompt_number": 10
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.13 Page No 172"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "#To calculate resultant AT/pole and peak air gap flux density, rotor AT/pole, stator AT and its angle with the resultant AT, stator currrent\n",
- "\n",
- "ph=3.0 \n",
- "S=36.0 \n",
- "c=8.0*2 \n",
- "p=4.0 \n",
- "f=50.0 \n",
- "N_ph=S*c/(ph*2) #turns/phase\n",
- "ga=180.0*p/S \n",
- "m=S/(p*ph) #slots/pole/phase\n",
- "\n",
- "#Calculations\n",
- "K_b=math.sin(math.radians(m*g/2.0))/(m*math.sin(math.radians(g/2))) #breadth factor\n",
- "V_L=400 \n",
- "V_ph=V_L/math.sqrt(3) \n",
- "phi_r=V_ph/(4.44*K_b*f*N_ph) \n",
- "print(phi_r,'phi_r(Wb/pole)') \n",
- "D=.16 \n",
- "l=0.12 \n",
- "PA=math.pi*l*D/4 #pole area\n",
- "B_rav=phi_r/PA \n",
- "B_rpeak=(math.pi/2)*B_rav \n",
- "g=2*10**-3 \n",
- "u_o=4*math.pi*10**-7 \n",
- "F_r=g*B_rpeak/u_o \n",
- "print(F_r,'F_r(AT/pole)') \n",
- "T=60 #torque(Nm)\n",
- "d=26 \n",
- "F2=T/((math.pi/2)*(p/2)**2*phi_r*math.sin(math.radians(d))) \n",
- "print(F2,'F2(AT/pole)') \n",
- "F1=math.sqrt(F2**2+F_r**2-2*F2*F_r*math.sin(math.radians(d))) \n",
- "print(F1,'F1(AT/pole)') \n",
- "w=math.degrees(math.acos((F1**2+F_r**2-F2**2)/(2*F1*F_r)))\n",
- "print(w,'angle(deg)') \n",
- "K_w=K_b \n",
- "I_a=F1/((3/2)*(4*math.sqrt(2)/math.pi)*K_w*(N_ph/p))\n",
- "\n",
- "#Results\n",
- "print(I_a,'I_a(A)') "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(0.01099635147629408, 'phi_r(Wb/pole)')\n",
- "(1823.0455139875667, 'F_r(AT/pole)')\n",
- "(1980.9832697544216, 'F2(AT/pole)')\n",
- "(2020.2729202496512, 'F1(AT/pole)')\n",
- "(61.80134857667341, 'angle(deg)')\n",
- "(47.44026875335716, 'I_a(A)')\n"
- ]
- }
- ],
- "prompt_number": 11
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.14, Page No 176"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "#to determine in F2,peak rotor AT, max torque, ele i/p at max torque(motoring mode),open ckt voltage(generating mode)\n",
- "\n",
- "print('motoring mode') \n",
- "K_w=.976 \n",
- "N_pole=746 \n",
- "p=4 \n",
- "I_f=20 \n",
- "\n",
- "#Calculations\n",
- "F2=(4/math.pi)*K_w*(N_pole/p)*I_f \n",
- "print(F2,'F2(AT)') \n",
- "B_r=1.6 \n",
- "D=.29 \n",
- "l=.35 \n",
- "T_max=(p/2)*(math.pi*D*l/2)*F2*B_r \n",
- "print(T_max,'T_max') \n",
- "f=50 \n",
- "w_m=4*math.pi*f/p \n",
- "P_in=T_max*w_m \n",
- "print(P_in,'P_in(W)') \n",
- "\n",
- "print('generating mode') \n",
- "m=S/(3*p) \n",
- "ga=180*p/S \n",
- "K_b=math.sin(math.radians(30))/(3*math.sin(math.radians(15.0/2))) \n",
- "K_w=K_b \n",
- "u_o=4*math.pi*10**-7 \n",
- "phi_r=((2*D*l/p)*(u_o/g))*F2 \n",
- "N_ph=20*p*4/2 \n",
- "E_ph=4.44*K_b*f*N_ph*phi_r \n",
- "E_l=math.sqrt(3)*E_ph \n",
- "\n",
- "#Results\n",
- "print(E_l,'E_l(V)') "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "motoring mode\n",
- "(4622.77627986085, 'F2(AT)')\n",
- "(2358.515712, 'T_max')\n",
- "(370474.781709765, 'P_in(W)')\n",
- "generating mode\n",
- "(11579.863937164595, 'E_l(V)')\n"
- ]
- }
- ],
- "prompt_number": 12
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.15, Page No 186"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# to find motor speed\n",
- "\n",
- "n=1500.0 #speed of sync generator\n",
- "p=4 \n",
- "f=n*p/120 \n",
- "\n",
- "#Calculations\n",
- "p_im=6.0 \n",
- "n_s=120*f/p_im \n",
- "s=0.05 #slip\n",
- "n_im=(1-s)*n_s \n",
- "\n",
- "#Results\n",
- "print(n_im,'speed of induction motor(rpm)') "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(950.0, 'speed of induction motor(rpm)')\n"
- ]
- }
- ],
- "prompt_number": 13
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.16, Page No 187"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "#to find voltage available b/w slip rings and its freq\n",
- "\n",
- "print('(a)') \n",
- "f=50.0 \n",
- "p=6.0 \n",
- "n_s=120*f/p \n",
- "n=-1000 \n",
- "\n",
- "#Calculations\n",
- "s=(n_s-n)/n_s \n",
- "f_s=f*s \n",
- "print(f_s,'slip freq(Hz)') \n",
- "v2=100 \n",
- "V2=s*v2 \n",
- "print(V2,'slip ring voltage(V)') \n",
- "\n",
- "print('(b)') \n",
- "n=1500 \n",
- "s=(n_s-n)/n_s \n",
- "f_s=abs(f*s) \n",
- "print(f_s,'slip freq(Hz)') \n",
- "v2=100 \n",
- "V2=s*v2 \n",
- "\n",
- "#Results\n",
- "print(V2,'slip ring voltage(V)') "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(a)\n",
- "(100.0, 'slip freq(Hz)')\n",
- "(200.0, 'slip ring voltage(V)')\n",
- "(b)\n",
- "(25.0, 'slip freq(Hz)')\n",
- "(-50.0, 'slip ring voltage(V)')\n"
- ]
- }
- ],
- "prompt_number": 14
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.18, Page No 197"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "#to find no of poles, slip and freq of rotor currents at full load, motor speed at twice of full load\n",
- "\n",
- "n_s=600.0\n",
- "f=50.0 \n",
- "P=120*f/n_s \n",
- "print(p,'no of poles') \n",
- "n=576.0 \n",
- "\n",
- "#Calculations\n",
- "s=(n_s-n)/n_s \n",
- "print(s,'slip') \n",
- "f2=s*f \n",
- "n_r=s*n_s \n",
- "print(n_r,'rotor speed wrt rotating field(rpm)') \n",
- "ss=f2*s \n",
- "n=(1-ss)*n_s \n",
- "print(n,'motor speed(rpm)') \n",
- "nn=528 \n",
- "s_old=s \n",
- "s_new=(n_s-nn)/n_s \n",
- "fac=s_new/s_old \n",
- "\n",
- "#Results\n",
- "print(fac,'factor is') "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(6.0, 'no of poles')\n",
- "(0.04, 'slip')\n",
- "(24.0, 'rotor speed wrt rotating field(rpm)')\n",
- "(552.0, 'motor speed(rpm)')\n",
- "(3.0, 'factor is')\n"
- ]
- }
- ],
- "prompt_number": 15
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 5.19, Page No 198"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "# to calculate amplitude of travelling wave mmf,peak value of air flux density, velocity of wave, current freq at some desired velocity\n",
- " \n",
- "K_w=.925 \n",
- "N_ph=48 \n",
- "I=750.0/math.sqrt(2) \n",
- "wndnglgth=2 \n",
- "wavelgth=wndnglgth/0.5 \n",
- "p=2*wavelgth \n",
- "\n",
- "#Calculations\n",
- "F_peak=(3.0/2)*(4*math.sqrt(2)/math.pi)*K_w*(N_ph/p)*I \n",
- "print(F_peak,'F_peak(A/m)') \n",
- "g=.01 \n",
- "u_o=4*math.pi*10**-7 \n",
- "B_peak=u_o*F_peak/g \n",
- "print(B_peak,'B_peak(T)') \n",
- "f=25 \n",
- "B=.5 \n",
- "v=f*B \n",
- "print(v,'velocity(m/s)') \n",
- "vv=72*10**3/3600 #given velocity\n",
- "f=vv/0.5 \n",
- "\n",
- "#Results\n",
- "print(f,'freq(Hz)') "
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(7949.789407440174, 'F_peak(A/m)')\n",
- "(0.9990000000000002, 'B_peak(T)')\n",
- "(12.5, 'velocity(m/s)')\n",
- "(40.0, 'freq(Hz)')\n"
- ]
- }
- ],
- "prompt_number": 16
- }
- ],
- "metadata": {}
- }
- ]
-}
\ No newline at end of file |