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25th January, 2006 ECE320, Spring 2006, Exam 1 Duration 1 hour Name PID Number Problem 1 2 3 Total SOLUTIONS Max Points 30 40 30 100 Points Instructions Read all the problems first. Attempt to solve first the problems you can do-don’t spend too much time on one problem. Read carefully the statement of the problems. Use the previous page’s back if more space is needed. Write neatly and show all the steps, no marks otherwise. Problem 1. For the circuit below, calculate the load I L using Thevenin’s theorem. j100 VS 12000 [V] A Ζ L 10 j10 Load j10 B IL j 200 j 20 Solution: The voltages at nodes A and B can be found by voltage division. Open Circuit Voltage ( VTH ) C j 10 -j 100 120 V A + -j 200 Vth - B j 20 D j 200 VAD 1200 j 200 j100 j 20 VBD 1200 j 20 j10 VTH VAB VAD VBD = 0. Thevenin Impedance ( ZTH ) 1 1 ZTH 1 1 1 1 j100 j 200 j10 j 20 ZTH j (66.66) j (6.66) j 60 Since VTH 0 , no voltage drop appears across terminals A and B; therefore, no current flows through Z L . IL VTH 0 Z TH Z L . Problem 2. For a balanced 3-phase circuit below, the source voltage is 208 V. Calculate (1) the real (active) and reactive power of each load, (2) the total real and reactive power of both loads, and (3) the real and reactive power provided by the source. Explain why the source reactive power differs from the total load reactive power. What about the source real power and the total load real power (should they be equal)? j0.2 ISa VSa IL2a IL1a VSb VSc 6 j6 2+ j2 Load 1 Load 2 Solution: Converting delta connected load to star and then considering only a single phase, the circuit will be as shown in figure. _____ j0.2 I sa _____ I La 2 _____ I La1 _____ AC Vsa 1200 (2 j 2) (2 j 2) (1) Total Impedance j 0.2 [(2 j 2) (2 j 2)] 2 j 0.2 __ I sa We have 1200 59.7 5.71 2 j 0.2 A __ 2 j2 I La1 I sa 42.2139.2 A 2 j2 2 j2 __ Using Current Division __ 2 j2 I La 2 I sa 42.21 50.7 A 2 j2 2 j2 __ Load Voltages __ __ __ __ V La1 I La1 2 j 2 119.4 5.72 V V La 2 I La 2 2 j 2 119.4 5.72 V Transmission Line Voltage Drop __ I sa j 0.2 11.9484.2 A Load 1 Real Power P L1 3V La1 I La1 cos 5.72 39.2 10.692 kW Reactive Power Q L1 3V La1 I La1 sin 5.72 39.2 10.692 kVAR Real Power P L 2 3V La 2 I La 2 cos 5.72 50.7 10.692 kW Reactive Power Q L 2 3V La 2 I La 2 sin 5.72 50.7 10.692 kVAR Load 2 (2) Total Real and Reactive Power of Both Loads: PTL P L1 P L 2 (10.69 10.69)kW 21.38 kW QTL Q L1 Q L 2 (10.69 10.69)kVAR 0 (3) The Real and Reactive Power Provided by the Source: P S 3V sa I sa cos 0 5.72 21.38 kW QS 3V sa I sa sin 0 5.72 2.138 kVAR Source Reactive Power differs from the total load reactive power (which is zero in this case) because it is the power associated with the transmission line. Transmission Line Reactive Power = 3 (11.94) (59.7) sin (84.2+5.72) = 2.138 kVAR Or = 3 (59.7 A)2 (0.2 ) = 2.138 kVAR Since, Transmission Line Real Power = 0 Therefore, Source Real Power = Total Load Real Power. Problem 3 In a 3-phase system below (Fig. a), the source is 230 V and the load (Load_1) is drawing 50 kW at 0.866 pf lagging. a) A second load (Load_2) is added and its real power is equal to 30 kW. What should the pf of the second load be in order for the total pf of the both loads together to be unity? b) Draw a power triangle diagram to represent the above-obtained real, reactive, and apparent power of the source, Load_1, and Load_2. Load_1 3-f Source Fig. a Load_1 3-f Source Fig. b Solution: (a) P L1 50 kW P f L1 0.866(lagging ) 50kW S L1 57.73 kVA 0.866 Q L1 57.73 sin(cos 1 0.866) 28.87 kVAR P L 2 30 kW [given] PTL P L1 P L 2 (50 30)kW 80 kW P f TL unity QTL Q L1 Q L 2 0 Q L1 Q L 2 Q L 2 28.87 kVA 28.87k 1 Q L 2 P f L 2 cos tan cos tan 1 30k P L 2 Therefore, P f L 2 0.72(leading ) , since Q L 2 0 Load_2 (b) Power Triangles 30 kW 57.73 kVA j28.8kVAR 41.6 kVA 50 kW Load 1 Load 2 -j28.8kVAR