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HW 04

Course: EE ee, Spring 2010
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4 ELEN3441FundamentalsofPowerEngineering Spring2011 Homework Solutions 4.1. (25 pt.) a) At no-load conditions, EA = VT = 240 V. The field current is given by VT 240 IF = = = 0.96 A Radj + RF 175 + 75 From Figure 5-1, this field current would produce an internal generated voltage EAo of 277 V at a speed no of 1200 r/min. Therefore, the speed n with a voltage of 240 V would be En EA 240 1200 n = n= A 0 = =...

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4 ELEN3441FundamentalsofPowerEngineering Spring2011 Homework Solutions 4.1. (25 pt.) a) At no-load conditions, EA = VT = 240 V. The field current is given by VT 240 IF = = = 0.96 A Radj + RF 175 + 75 From Figure 5-1, this field current would produce an internal generated voltage EAo of 277 V at a speed no of 1200 r/min. Therefore, the speed n with a voltage of 240 V would be En EA 240 1200 n = n= A 0 = = 1040 rpm 277 E A0 n0 E A0 b) The minimum speed will occur when Radj = 100 , and the maximum speed will occur when Radj = 400 . The field current when Radj = 100 is: VT 240 IF = = = 1.37 A Radj + RF 100 + 75 From the magnetization curve, this field current would produce an internal generated voltage EAo of 289 V at a speed no of 1200 r/min. Therefore, the speed n with a voltage of 240 V would be En EA 240 1200 n = n= A 0 = = 997 rpm 289 E A0 n0 E A0 The field current when Radj = 400 is: VT 240 = = 0.505 A Radj + RF 400 + 75 From the magnetization curve, this field current would produce an internal generated voltage EAo of 207 V at a speed no of 1200 r/min. Therefore, the speed n with a voltage of 240 V would be En EA 240 1200 n = n= A 0 = = 1391 rpm 207 E A0 n0 E A0 IF = c) The starting current of this machine (ignoring the small field current) is V 240 I L , start = T = = 1263 A RA 0.19 The rated current is 110 A, so the starting current is 11.5 times greater than the full-load current. This current is extremely likely to damage the motor. 4.2. (25 pt.) a) The output power of this motor at full load is Pout = 15 746 = 11190 W The input power is Pin = VT I L = 120 115 = 13800 W Therefore the efficiency is Page|1 ELEN3441FundamentalsofPowerEngineering = Spring2011 Pout 11190 100% = 100% 81% 13800 Pin b) If the armature current is 50 A, then the input power to the motor will be Pin = VT I L = 120 50 = 6000 W The internal generated voltage at this condition is E A 2 = VT I A ( RA + RS ) = 120 50 ( 0.1 + 0.08 ) = 111V and the internal generated voltage at rated conditions is E A1 = VT I A ( RA + RS ) = 120 115 ( 0.1 + 0.08 ) = 99.3 V The final speed is given by the equation since the ratio EAo,2 /EAo,1 is the same as the ratio 2/1. Therefore, the final speed is EE n n = A 2 Ao ,1 1 E A1 E Ao ,2 The internal generated voltage EAo,2 for a current of 50 A and a speed of n0 = 1200 r/min is EAo,2 = 129V, and the internal generated voltage EAo,1 for a current of 115 A and a speed of n0 = 1200 rpm cannot be determined from the curve but will be approximated as EAo,1 = 155 V. E E n 111 155 1050 = 1410 rpm n = A 2 Ao ,1 1 = 99.3 129 E A1 E Ao ,2 The power converted from electrical to mechanical form is Pconv = E A I A = 111 50 = 5550 W The core losses in the are motor 420 W, and the mechanical losses in the motor are 3 Pmech 3 n 1410 = 2 460 = 460 = 1114 W 1050 n1 Therefore, the output power is Pout = Pconv Pmech Pcore = 5550 1114 420 = 4016 W and the efficiency is = Pout 4016 100% = 100% 67% 6000 Pin 4.3. (25 pt.) These computations must be performed for armature currents of 25.3 A, 50.7 A, 76 A, and 101.3 A. Page|2 ELEN3441FundamentalsofPowerEngineering Spring2011 If IA = 25.3 A, then E A = VT I A ( RA + RS ) = 240 V 25.3 A ( 0.09 + 0.06 ) = 236.2 V The mmf is = NI A = 33 25.3 A = 835 A turn that produces a voltage EA0 of 134 V at n0 = 900 rpm. Therefore, the speed of the motor at these conditions is n= EA 236.2 V n0 = 900 = 1586 rpm E A0 134 V The power converted from electrical to mechanical form is Pconv = E A I A = 236.2 V 25.3 A = 5976 W Since the rotational losses are ignored, this is also the output power of the motor. The induced torque is ind = Pconv m = 5976 W = 36 N m 1586 rpm 2 60 Similar computations for other armature currents lead to the following results: IA (A) 25.3 50.7 76 101.3 n (rpm) 1586 1062 899 803 Pconv (W) 5976 11780 17370 22770 ind (Nm) 36 106 185 271 4.4. (25 pt.) The rated line current of this motor is 60 A, and the rated armature current is IA = IL IF = 60 A 6 A = 54 A. The maximum desired starting current is (2.5)(54 A) = 135 A. Therefore, the total initial starting resistance must be 240 RA + Rstart ,1 = = 1.778 135 Rstart ,1 = 1.778 0.12 = 1.658 The current will fall to rated value when EA rises to E A = 240 1.658 54 = 150.5 V At that time, we want to cut out enough resistance to get the current back up to 135 A. Therefore, 240 150.5 RA + Rstart ,2 = = 0.663 135 Rstart ,2 = 0.663 0.12 = 0.543 With this resistance in the circuit, the current will fall to rated value when EA rises to E A = 240 0.543 54 = 210.7 V Page|3 ELEN3441FundamentalsofPowerEngineering Spring2011 At that time, we want to cut out enough resistance to get the current back up to 185 A. Therefore, 240 210.7 RA + Rstart ,3 = = 0.217 135 Rstart ,3 = 0.217 0.12 = 0.097 With this resistance in the circuit, the current will fall to rated value when EA rises to E A = 240 0.217 54 = 228.3 V If the resistance is cut out when EA reaches 224.6 V, the resulting current is 240 228.3 IA = = 97.5 A < 135 A 0.12 so there are only three stages of starting resistance. The three stages of starting resistance can be found from the resistance in the circuit at each state during starting. Rstart ,1 = R1 + R2 + R3 = 1.658 Rstart ,2 = R2 + R3 = 0.543 Rstart ,3 = R3 = 0.097 Therefore, the starting resistances are R1 = 1.115 R2 = 0.446 R3 = 0.097 Page|4
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