In any electrical device, including capacitors, when we apply a certain amount of total power (energy) into the device, we get a lesser amount out of it. The difference between the amounts in and out is "lost" or used within the device and is referred to as the "power loss." If we now divide this "power loss" by the input power, the resulting ratio figure is the "power factor" of the device. The "power factor" (PF) then is a direct measure of the "inefficiency" of a capacitor, in that it supplies us with a measuring tool to determine how much of the total power sup­plied to a capacitor is used by the capacitor itself and therefore not available to do otherwise "use­ful" work.

Before proceeding further, a review of some fund­amental concepts relative to the application of a sine wave voltage to a capacitor will be helpful.

Although a capacitor is primarily capacitive in na­ture, it does possess very small distributed a­mounts of resistive and inductive elements. These distributed resistor and inductor elements can be lumped into a single value for computation pur­poses as shown in the following equivalent circuit.

Note also that since R, L, and Care in series in our circuit, the circuit current (I) is the same current that passes through all elements {in magnitude) and therefore:

With the element currents out of phase with the voltages, Ohm's Law must be modified to use im­pedances and reactances in addition to resistance. That is —

The power relationship of our circuit is:

Drawing the vector relationship, our power equa­tion is:

POWER FACTOR

The "power loss" within the capacitor is that portion of the total power applied to the capacitor that is not stored by the capacitor on an instantaneous basis. As the current passes through the series resistance element, it generates heat and this then is the "power loss" we are concerned with. It should be noted here that all energy losses (due to leads, dielectric polarization, connections, and eddy cur­rents in the electrode material) are taken into ac­count by the "equivalent series resistance" ele­ment. Analysis of the power equation shows:

We can readily see that if X and Z are practically identical (which would be the case when o ap­proaches 90°), then the PF and OF would also be practically identical.

For any given unit, an analysis of the divergence error in the equation DF=PF shows:

We see that for all values of OF=.1 O (10% OF) or less, the error in the assumption DF= PF will be .5% or less.

The reason for using DF as a parameter instead of PF is that determination of PF values requires much more complicated equipment and proced­ures compared to the simple comparison tech­nique used for measuring DF.

DF then is a convenient, somewhat artificial method by which the "inefficiency" of a capacitor can be noted.

Q (Factor of Merit)

The "Q" or "Factor of Merit" of a device is also an artificial measurement that will conveniently allow notation of the "inefficiency" (or power losses) of that device.

By definition, a is the ratio of the reactance to the series resistance. This then shows the following relationship:

or: a is the reciprocal of the DF. For instance:

Common usage pretty much boils down to this:

1. "Power Factor" is used for capacitors when the PF is 10% or greater.
2. "Dissipation Factor" is used when the PF is less than 10%.
3. "Q" is occasionally used for capacitors. It is widely used for inductors and total circuits.