3 phase power measurement
DESCRIPTION
ElectricalTRANSCRIPT
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UNIVERSITY OF TECHNOLOGY, JAMAICA
Faculty of Engineering & Computing
School of Engineering
Electrical Machine
Lab #1: Two Wattmeter Method of Measuring Power in Three
Circuits
In partial fulfilment of the requirement for the
Bachelor of Engineering Degree
Date: February 4, 2010
Ainsloy Richards (Id#:0703146)
Instructor: Nathan Martin
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Objective
To test the theory that the sum of the two wattmeter readings gives the total power in a
three phase balanced load and to compare the experimental value of the power with the
theoretical value.
Theory
General
Balance in a three phase load is achieved when the line voltages are equal and the line
currents are equal. For a balanced three phase system that is connected in wye, the line currents
are equal and line voltages are equivalent to the product of root three and the phase voltage
{( and . On the contrary, the line current is equivalent to the product ofroot three and the phase current and the line voltages are equal to the phase voltages in a delta
connection ( { ( .
Power
The apparent power for each phase in a three system is given by:
, for the delta connection:
Hence, the apparent power in the three phase delta system is given by:
The total active power in a three phase system is three times the product of the phase voltage,
phase current and the power factor ().
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That is;
For the both delta and Wye connection is; For a purely resistive circuit, the power factor is equal to 1 ( ) and the total power isequal to the apparent power.
The power in a three phase system can be measured by using the one wattmeter meter or the two
wattmeter method. The one wattmeter method is limited to measuring power in the star
connection but the two wattmeter method is used for both the star and delta connection. The total
power in the three phase system, when using the two wattmeter method, is given by the algebraic
sum of the power on both meters.
That is; Apparatus
3 Ammeter, 0-5 A 2 Electronic Wattmeter 68 - 200W
3Bulbs, 150 W/ 220V Digital Multimeter (DDM)
Universal Power Supply 60 -105 Three Phase Measurement Panel
Fig. 1 Experimental Circuit
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Procedure
The circuit was setup a shown in figure 1 and the universal power supply switched on.
The variable supply was adjusted to give a reading of 110 V between the red and yellow line.
The line voltages was then measured and recorded. The voltage drop across each phase, the
phase currents, and the line currents were also measured and recorded. The universal power
supply was the switched off and the circuit dissembled.
Results
Table 1a: The necessary data that was collected in the experiment for power calculation
Line
Voltages
(V)
Line
Currents
(A)
Phase
Currents (A)
Phase
Voltages (V)
Measured
Power (W)
Calculated
power (W)
W1 W2
VRY= 110 IR= 0.4375 IRY= 0.24 VRY= 110
50 58
26.4
VYB= 114 IY= 0.45 IYB= 0.25 VYB= 114 28.5
VBR = 113 IB= 0.4625 I BR= 0.2375 VBR= 113 26.8
Total power 108 81.7
Sample Calculations:
Since the circuit was not balanced, the power in each phase must be calculated separately by the
equation;
(Assuming that the loads are purely resistive)For; VRY= 110 V, IRY= 0.24 A
The Power Factor
Taking the average of the line voltages and phase currents and assuming that the system is
balanced.
(
)
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(
)The Total power is by;
The Power factor using the readings from the Wattmeters:
[ ] * +*
+
Discrepancy between the measured and calculated power;
( )
Discussion:
The power in consumed in a three-phase delta or wye connection can be found by the two
wattmeter method. This is achieved by using one of the lines as reference (connected in to the
voltage coil of both wattmeters) and the remaining lines are connected to current coil of the
wattmeters. The experimental value for the total power that was consumed in the three phase
circuit was calculated by the algebraic sum of the power reading on wattmeter 1 and 2. The
dissipated power was found to be 108 W. In theory, the dissipated power in the balanced three-
phase system is three times the power consumed in a single phase. The theoretical power was
calculated to be 81.7 W. When the theoretical and experimental values for the power are
compared, it is revealed that there is a significant 32.2 % discrepancy in the readings and it is
apparent that the experiment did not support the theory. This experiment can be considered as
been unsuccessfully conducted due to the fact that the experimental power is greater that the
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theoretical power. In general, the theoretical values for the power should be greater since it takes
into consideration the ideal situation. It does not take into consideration the resistance of the
wire and the addition resistance associated with the attaching the measuring apparatus to the
system that would have cause the experimental value to be less. The only logical reason for the
having the measured power greater than the theoretical power is that the apparatus used were
faulty. The apparatus must have not been calibrated before the start of the experiment. It must
also be noted that the system was not balanced and this could have contributed to the discrepancy
in the result.
Conclusion:
The experimental power consumed by the system was found to be 108 W and the
theoretical power consumption is 81.7 W. There is a 32.2% deviation of the experimental power
form the theoretical power but due to the source of error encountered in the experiment, it can
still be stated that the total power in the system is the sum of the power reading on both
wattmeters.
Reference
Wildi, T, 2006, Electrical Machines, Drives and Power System, 6th
Edition, Prentice Hall
McPherson, L, 2003, An Introduction to Electrical Machines and Transformers, 2nd
Edition, John
Wiley & son
Milton, R, 2010, lesson_1_Three Phase BEng 3m lecture notes,
http://utechonline.utech.edu.jm/course/view.php?id=413