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Three Phase AC Power Measurements - Laboratory Experiment 5 | ECE 225, Lab Reports of Electrical Circuit Analysis

Material Type: Lab; Class: Circuit Analysis and Design; Subject: Electrical & Computer Engineer; University: Boise State University; Term: Unknown 1989;

Typology: Lab Reports

Pre 2010

Uploaded on 08/19/2009

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koofers-user-s09 🇺🇸

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Download Three Phase AC Power Measurements - Laboratory Experiment 5 | ECE 225 and more Lab Reports Electrical Circuit Analysis in PDF only on Docsity! Boise State University Department of Electrical and Computer Engineering ECE225L – Circuit Analysis and Design Lab Experiment #5: Three-Phase AC Power Measurements 1 Objectives The objectives of this laboratory experiment are: • to verify voltage and current relationships in balanced three-phase AC circuits • to measure three-phase real power using the two-wattmeter method. 2 Theory We are all familiar with single-phase AC circuits, particularly for domestic uses. The number of phases encountered in a power circuit should not be confused with the number of different voltages available from the source. For example, domestic 120/240-volt sources are only one phase since they are usually obtained from one phase of a three-phase electric power distribution network. Three-phase power circuits are predominant in commercial and industrial uses, mostly for eco- nomic reasons although the very existence of three-phase circuits can be attributed to their ease of creation by a three-phase AC generator. In terms of output power, a polyphase circuit is somewhat like a multicylinder internal combustion engine. The power in all cylinders is summed to obtain the total shaft power but the construction is such that each cylinder is important because the power portion of the engine stroke does not occur at the same time in each cylinder. The total real and reactive power delivered to or consumed by a load is the algebraic sum of that consumed by each element regardless of the type of connection (Y or ∆). Three-phase real and reactive power consumption may be measured in many ways. This experiment uses the classical two-wattmeter method for the total three-phase real power. A wattmeter is essentially a stationary ammeter coil (current coil) coupled with a movable voltmeter coil (potential coil) in series with a very large resistance. The average value of the torque produced between the two coils is calibrated to read the average power in watts on the deflection scale. The wattmeter, when placed between a source and a load, reads the following wattage: W = |Ṽ ||Ĩ| cos(6 Ṽ − 6 Ĩ) (1) where |Ṽ | is the rms magnitude of the voltage across the potential coil, |Ĩ| is the rms magnitude of the current through the current coil, and (6 Ṽ − 6 Ĩ) is the phase shift between the voltage across the potential coil and the current through the current coil. 3 Equipment • OrCAD PSpice Version 9.1 or 9.2. 1 − + − + − + N 208 Vrms 3−wire 3−Phase C B A 50 Ω + ~ C I ~ B I ~ A I − A W C W − 50 Ω 50 Ω Figure 1: Balanced Y-connected Resistive Load 4 Procedure Part A: Balanced Y-Connection Step 1: Simulate the balanced Y-connected resistive load shown in Figure 1 using PSpice. You can use either three line-to-neutral voltage sources displaced by 120o or you can use two line-to- line voltage sources. In this latter case, there is no need for a third line-to-line voltage source. (Why?) Step 2: Record the following measurements after activating the pair of cursors in PSpice: IA,pp (A) IB,pp (A) IC,pp (A) VAN,pp (V) VBN,pp (V) VCN,pp (V) VAB,pp (V) VBC,pp (V) VCA,pp (V) Step 3: Submit a plot showing the amplitudes and phase shifts of the three line currents iA(t), iB(t), iC(t), a plot showing the three line-to-neutral voltages vAN (t), vBN (t), vCN (t), and a plot showing the three line-to-line voltages vAB(t), vBC(t), vCA(t). Step 4: Submit a plot showing the phase shift between the the voltage vAB(t) and the current iA(t), and a plot showing the phase shift between the voltage vCB(t) and the current iC(t). Record these two phase shifts below: VAB,pp (V) IA,pp (A) ∆t1 (ms) VCB,pp (V) IC,pp (A) ∆t2 (ms) 2
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