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The two-wattmeter method for measuring power in balanced 3-phase systems, including 4-wire and 3-wire configurations. It covers predicting and measuring line and line-to-neutral voltages, line currents, and total power using the two-wattmeter approach. The document also discusses phase shift measurement methods using an oscilloscope.
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The three-phase circuit studied in this lab is represented in Fig. 1. While the load can be either Y- or ∆-connected, through Y-∆ transformation, the load has an equivalent Y representation. The source will either by Y (208 Vac) or ∆ (240 Vac). For this figure, the source is Y connected.
3-phase Load
(^3 3 )
(^3 3 )
3 3 3
Z
LN L L L
S P jQ
S S S
S V I V I
φ (^) φ φ
φ (^) φ φ
φ
Z YEQ = ZYEQ θ Z
where θ Z = −θ
where V = V
Figure 1: 3-phase circuit.
The 208 source does not come directly from the utility room (where the ALBs reside), but rather from the service entrance to the building. The 208 outlet at the station wall is always “hot”, assuming no breakers have been tripped. When this 208 source is connected to the back panel, and through the metered 3φ breaker on the bench front panel, the neutral is connected to the ground of the bench.
The 240 source comes directly from the utility room at the output of a 75 kVA 3φ Y- ∆ , 480-to-240 Vrms transformer. Sometimes, the secondary winding of one of the phases has the center of the winding tapped, giving the user a fourth wire, which can be connected to ground. This is not the case for our transformer. Hence, there are only three wires, each being one phase of the output of the transformer. The 240 outlet at the station wall only becomes “hot”, when a contactor is closed within the
3-phase Load Resistive, Inductive, Capacitive
Figure 2: Two-Watt Meter method for measuring power in a 3-phase circuit.
With the meters connected as such, assuming that VAC = VBC = VL ,
and that the total power to the 3φ load is
P 3 (^) φ = W 1 (^) + W 2 (4)
The proof for this follows below.
PROOF: The Fluke 41 meter essentially computes power according to:
1
Re ,
120 30
AC A
AC CA L A L
2
Re ,
120 30 120
BC B
BC L B L
Q.E.D.
Here, we see that if the load is purely real, the inherent 30 degree phase shift is easily seen between the line current and the respective line voltage.
approaches 0 and W 1 approaches
V I. If θ leads by as much as 60 degrees
(capacitive load), W 1 approaches 0 and W 2 approaches
V IL L. If the pf angle
increases beyond 60 degrees (lag or lead), one wattmeter will become negative and the other will remain positive – and this is perfectly ok
The important observation to realize is that when real power is held constant and the reactive load is uniformly increased or decreased,
, i.e., don’t be in a hurry to switch the current probe around just to obtain a positive power reading – in the end, the power readings from each meter are added together to obtain the total power delivered to the load.
constant and the true value for the total power delivered to the load is obtained.
is when θ is 0 degrees, i.e., pf=1 (pure resistive). Hence, when pf = 1,.
P 3 (^) φ = W 1 + W 2 = 0. This is expected, since the load is purely reactive. This begs the question then … “Is there a simple equation that gives you Q when given W 1 (^) and W 2 measurements?” The answer is yes (in the ideal situation – perfect measurements) and the equation is given by:
Turn the power on. The meter will indicate if indeed you have the correctly identified A, B, and C lines. Try switching the leads from the meter between two phases – what did you notice? Turn the power off.
DRAW A CIRCUIT DIAGRAM IN YOUR NOTEBOOK showing the Y-connected source and ∆-connected load.
NOTE: since the load is ∆-connected, the system is actually a 3-wire system. If a load with a ground is introduced to the system, then the circuit becomes a 4-wire system
2 3 3
L per phase
φ R
To determine the 3-phase power level the ALB must be set to, apply this formula:
.
Once the total power level is determined, you should turn the power on and place the ALB in closed-loop mode, and confirm your setting at the LabVIEW meters. Place the ALB in open-loop mode, and turn the power off
Predict the phase and RMS value of VBC
with respect to (WRT) VAB
(i.e., trigger off channel connected to VAB
a) Connect the differential probes to the power supply side for measuring VBC
and VAB
. Set probe values correspondingly. Turn the power on and place the ALB in closed-loop mode.
Implement both phase shift measurement methods.
For METHOD 1, use cursors to measure the amplitudes of each voltage, and convert these values to their RMS values. Save data and produce plots to be placed in your notebook. Compare each of these methods to your predicted values.
Place the ALB in open-loop mode, and turn the power off
b) Connect the current probe to phase A line between Y-source and ∆-load, with arrow pointing towards the load (i.e., ALB). Set probe to values corresponding to expected current magnitudes.
Predict the RMS value of Line A current and its phase WRT
(consider (2) … hmmm.) Display on the oscilloscope only VAB
and IA
Using both phase shift measurement METHODS 1 and 2 to make the appropriate measurements for (^) IA
, with respect to (^) VAB
. Save data and produce plots to be placed in your notebook. Place the ALB in open-loop mode, and turn the power off.
Predict the RMS value of Line A current and its phase WRT VAN
Display on the oscilloscope only (^) VAN
and (^) IA
Using one of the METHODS 1 or 2, as described above, make the appropriate measurements for IA
, with respect to VAN
. Save data and produce plots to be placed in your notebook.
Place the ALB in open-loop mode, and turn the power off
DRAW A CIRCUIT DIAGRAM IN YOUR NOTEBOOK showing the Y-connected source, in-line inductors, and ∆-connected load.
a) With power off, place an inductor in each line between the input and the ALB. Set the reactances to 10 Ω.
By the method of converting the ∆-connected resistance (ALB) of 60 Ω to an equivalent Y-load, use the single phase equivalent circuit to compute the expected line current (phase and magnitude WRT VAN
for this configuration.
for this configuration).
Turn the power on and place the ALB in closed-loop mode.
Use METHOD 2 for phase measurements and confirm these values.
Place the ALB in open-loop mode, and turn the power off.
Referring to Fig. 2, use the Fluke 41 for conducting the two-watt meter approach to confirm this prediction.
Estimate the value for W1 and W2, using (2) and (3).
Turn the power on and place the ALB in closed-loop mode and record W1 and W2.
Compare results of a) W1 to estimated result (2) b) W2 to estimated result (3) c) (4) to predicted result (1.b) d) (5) to predicted result (1.c)
b) The VAR computation (5) may have the most error compared to the error in (4). Explain. c) Adjust the decade reactance box to successively larger or smaller values. At each increment/decrement, record W 1 and W 2 and note the direction each measurement is taking, i.e., is the value increasing or is it decreasing towards a negative value. Explain to your lab instructor what pattern develops and why. Do you expect that W1 or W2 to change sign? How should each measurement change as the reactance is adjusted? Explain to your instructor.
Turn the power on. The meter will indicate if indeed you have the correctly identified A, B, and C lines. Try switching the leads from the meter between two phases – what did you notice? Turn the power off.
DRAW A CIRCUIT DIAGRAM IN YOUR NOTEBOOK showing the ∆-connected source and ∆-connected load.
To determine the 3-phase power level the ALB must be set to, apply this formula:
2 3 3
L per phase
φ R
Once the total power level is determined, you should turn the power on and place the ALB in closed-loop mode, and confirm your setting at the LabVIEW meters. Place the ALB in open-loop mode, and turn the power off
Predict the phase and RMS value of VBC
with respect to (WRT) VAB
(i.e., trigger off channel connected to VAB
a) Connect the differential probes to the power supply side for measuring VAB
and (^) VBC
. Set probe values correspondingly. Turn the power on and place the ALB in closed-loop mode.
Implement both phase shift measurement methods.
For METHOD 1, use cursors to measure the amplitudes of each voltage, and convert these values to their RMS values. Save data and produce plots to be placed in your notebook. Compare each of these methods to your predicted values.
Place the ALB in open-loop mode, and turn the power off
b) Connect the current probe to phase A line between Y-source and ∆-load, with arrow pointing towards the load (i.e., ALB). Set probe to values corresponding to expected current magnitudes.
Predict the RMS value of Line A current and its phase WRT
? (consider (2) … hmmm.)
Display on the oscilloscope only VAB
and IA
Using both phase shift measurement METHODS 1 and 2 to make the appropriate measurements for IA
, with respect to VAB
. Save data and produce plots to be placed in your notebook. Place the ALB in open-loop mode, and turn the power off.
Place the ALB in open-loop mode, and turn the power off.
c) Adjust the decade reactance to successively larger or smaller values. At each increment/decrement, record W 1 and W 2 and note the direction each measurement is taking, i.e., is the value increasing or is it decreasing towards a negative value. Explain to your lab instructor what pattern develops and why. Do you expect that W1 or W2 to change sign? How should each measurement change as the reactance is adjusted? Explain to your instructor.
DRAW A CIRCUIT DIAGRAM IN YOUR NOTEBOOK showing the Y -connected source, in-line inductors, and ∆-connected load.
a) With power off, place three capacitors in a Y-configuration in parallel with the ALB. Connect the neutral of the capacitive Y-load to ground. Set the capacitive reactances to 110 Ω. By the method of converting the ∆-connected resistance (ALB) of 80 Ω to an equivalent Y-load, use the single phase equivalent circuit to compute the expected line current (phase and magnitude WRT VAN
for this configuration.
Turn the power on and place the ALB in closed-loop mode.
Using a current probe to see if the neutral current is relatively small compared to each capacitor current? If it is (which is to be expected since the ∆-source is does not have a tap to ground), then proceed with all measurements WRT V AN
If it is not, then turn power off, remove the neutral from ground, and make all measurement WRT VAB
Use METHOD 2 for phase measurements and confirm these values.
Place the ALB in open-loop mode, and turn the power off.
Referring to Fig. 2, use the Fluke 41 for conducting the two-watt meter approach to confirm this prediction.
Estimate the value for W1 and W2, using (2) and (3).
Turn the power on and place the ALB in closed-loop mode and record W1 and W2.
Compare results of a) W1 to estimated result (2)
b) W2 to estimated result (3) c) (4) to predicted result (1.b) d) (5) to predicted result (1.c)
b) The VAR computation (5) may have the most error compared to the error in (4). Explain. c) Adjust the decade reactance box to successively larger or smaller values. At each increment/decrement, record W 1 and W 2 and note the direction each measurement is taking, i.e., is the value increasing or is it decreasing towards a negative value. Explain to your lab instructor what pattern develops and why. Do you expect that W1 or W2 to change sign? How should each measurement change as the reactance is adjusted? Explain to your instructor.
Present your data with tables including percent error calculations and phasor diagrams showing the 30o^ and 120o^ phase shifts throughout the system.
Also, be sure to answer questions that were asked throughout the procedure.
You may also want to work the extra credit.