EE311 - Power factor correction


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Title: Power factor correction
Aim:
1. To show the relationship between power, power factor and volt-amps.
2. To correct the power factor using power factor correction capacitors.

Apparatus: See your laboratory manual for the apparatus.

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THEORY:

A. Power Triangle

The apparent power is the vector sum of real and reactive power. As shown in Figure 1, the power triangle has the following components
1. Real power or active power (P) watt [W]
2. Reactive power (Q) volt-amperes reactive [Var]
3. Complex power (S)
4. Apparent Power (|S|) that is, the absolute value of complex power S volt-ampere [VA]
5. Impedance angle (φ) the angle of difference (in degrees) between voltage and current; Current lagging Voltage (Quadrant I Vector), Current leading voltage (Quadrant IV Vector)

Reactive power does not transfer energy, so it is represented as the imaginary axis of the vector diagram. Real power moves energy, so it is the real axis.


B. Power factor

The ratio between real power and apparent power in a circuit is called the power factor. It's a practical measure of the efficiency of a power distribution system. For two systems transmitting the same amount of real power, the system with the lower power factor will have higher circulating currents due to energy that returns to the source from energy storage in the load. These higher currents produce higher losses and reduce overall transmission efficiency. A lower power factor circuit will have a higher apparent power and higher losses for the same amount of real power.
The power factor is one when the voltage and current are in phase. It is zero when the current leads or lags the voltage by 90 degrees. Power factors are usually stated as "leading" or "lagging" to show the sign of the phase angle, where leading indicates a negative sign.
Purely capacitive circuits cause reactive power with the current waveform leading the voltage wave by 90 degrees, while purely inductive circuits cause reactive power with the current waveform lagging the voltage waveform by 90 degrees. The result of this is that capacitive and inductive circuit elements tend to cancel each other out.
Where the waveforms are purely sinusoidal, the power factor is the cosine of the phase angle (φ) between the current and voltage sinusoid waveforms. Equipment data sheets and nameplates often will abbreviate power factor as "cosφ" for this reason.
C. Power Factor correction

Most industrial loads (motors, lights, etc.) are inductive in nature, so they have a lagging power factor. Therefore, these loads draw more current (apparent power) than is required to do the actual work (real power). This results in higher costs to the customer.
In the below example, a load is simplified to its electrical equivalents. The load requires a current IL to run, so the source must supply it.
Power Factor Correction attempts to improve the power factor by the addition of capacitor(s) in parallel with the load. These capacitors supply some or all of the reactive power to the inductive load, which reduces the reactive power and therefore the current that the power supply delivers. In this second circuit, the load still requires a current IL to run, but some of the current is coming from the capacitor, so the current the source must supply is less.

For Procedure and Circuit Diagram, See your Electrical Laboratory Manual on page 3. 

 Fill Up Tables in Your Manual and Continue To….

PRECAUTIONS:
For Precautions, See General Electrical Lab Precautions

Answers to Questions:
No Questions in this experiment.

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About Stephen Djes

Stephen Djes is a passionate Graduate of Engineering from the University of Benin, and he is geared towards helping fellow engineering students in the great institution of UNIBEN to do better at academics.
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