Checking this Equation for Power Factor

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Discussion Overview

The discussion revolves around the equation for power factor in electrical systems, particularly in the context of AC generators and their ratings in kVA versus kW. Participants explore the implications of power factor, including displacement and distortion, and how these relate to the performance and specifications of generators.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Experimental/applied

Main Points Raised

  • One participant presents an equation for power, incorporating power factor and total harmonic distortion (THD), suggesting it as a roadmap for understanding generator ratings.
  • Another participant defines displacement power factor and distortion power factor, providing formulas for their calculation and discussing their relationship to total power factor.
  • A different participant notes that synchronous generators can exhibit a wide range of power factors, emphasizing that only the apparent power (VA, kVA) is consistently defined, while real power (W, kW) can vary based on load conditions.
  • One participant expresses a desire to explain the concept of power factor to a friend, suggesting a tailored approach to clarify the differences between DC and AC power calculations.
  • Another participant critiques the common assumption that power factor applies only to sinusoidal waveforms, providing a more general definition based on instantaneous power delivery.
  • Participants discuss the implications of power factor on generator performance, including the potential for damage if operated under inappropriate load conditions, and the importance of understanding minimum power factor limits specified by manufacturers.
  • One participant shares a personal anecdote about a generator that was damaged, speculating on the causes related to power factor and load conditions.
  • Another participant highlights the financial implications for industrial customers charged for both real energy consumption and power factor, noting the additional heating effects in electrical components.

Areas of Agreement / Disagreement

Participants express various viewpoints on the definitions and implications of power factor, with some agreeing on the importance of understanding both displacement and distortion factors, while others raise concerns about the assumptions made regarding sinusoidal waveforms and the operational limits of generators. The discussion remains unresolved with multiple competing views presented.

Contextual Notes

Participants acknowledge that the definitions and calculations of power factor can depend on specific conditions and assumptions, such as the nature of the load and the waveform characteristics. There are also references to unresolved mathematical steps and the need for clarity on the implications of power factor in practical applications.

Who May Find This Useful

This discussion may be useful for electrical engineering students, professionals working with generators, and individuals interested in understanding the complexities of power factor in AC systems.

Guineafowl
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TL;DR
Is my expression for real power in an AC circuit, including distortion and displacement, valid? I’m almost certain it is, but just checking I’m not missing anything.
$$P=IV \left [ \frac {cos\phi} {\sqrt{1+THD^2}} \right ]$$

The reason for asking is, I can’t find the equation written out in full like this.

A friend wants to know why his generator is rated in kVA. Having done basic school physics, he’s familiar with P=IV in the DC steady state, so is expecting kW.

I was thinking the equation above would be a useful starting point, a sort of roadmap to point at, allowing me to pick out the term in square brackets, and deal with displacement PF and distortion PF using the top and bottom terms inside, respectively.
 
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PF = displacement power factor
θ = Difference between the phase of the voltage and the phase of the current (phase displacement) in degrees.
The distortion power factor is calculated as follows:
PFTHD=1/sqrt(1+TDH)
Then total power factor =PF*PFTHD=cos(θ)/sqrt(1+THD^2)
The power now will be:
I*V* cos(θ)/sqrt(1+THD^2)
 
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The synchronous generator- as a transformer also-may present any value of power factor from -1 to +1 then P=I*V*cos(θ) [in W ,kW or MW] may be any value from +V*I up -V*I so, only V*I [VA, kVA or MVA] does make sense.
 
Thanks, so the equation as presented is correct, it seems. Oddly, I’ve never seen it written out in full.

With this chap, I thought I’d tailor the answer to his level of understanding, perhaps as follows:

With DC, P=IV, in watts. With AC, you have [post #1 equation], with the extra term because certain loads behave like bigger loads than they actually are. The extent to which they do this is measured by their power factor:
$$PF = \left [ \frac {cos \phi} {\sqrt {1+THD^2}} \right ]$$

Then go for ##cos\phi## leading/lagging, power triangle, brief bit on non-linear loads to cover THD.

With that in mind, the generator (or transformer) maker doesn’t know what load you’re driving, and therefore how much useful power you’re going to get out of it. So as you can see, particularly from the power triangle, they state their machine can make “this much” kVA, and leave you to work out the available, useful kW your load will get out of that, using the PF.


Something like that, anyway. The internet, wikipedia, etc are great resources, but sometimes an answer tailored to you is nice. It’s also nice to explain something well to someone, and watch their face as the penny drops.
 
Much of what you see about power factor assumes sinusoidal wave forms. This is a common application and OK, but it's not the real definition. The real definition is conceptually simple, it's the ratio of power actually delivered to the load (the instantaneous product of voltage and current) to the product of the rms voltage and the rms current. The latter is the power that would have been delivered to a resistive load with that output.

$$ PF = \frac{1}{T} \int_0^T v(t)i(t) \, dt ~~/~~(V_{rms} I_{rms}) $$

The RMS (root mean square) operator is ## \sqrt{\frac{1}{T} \int_0^T f(t)^2 \, dt} ## it is a description of the power that would be dissipated in a resistor exposed to that voltage or current.

## \frac{1}{T} \int_0^T v(t)i(t) \, dt ## is expressed as Watts

## V_{rms} I_{rms} ## is expressed as VA

VA is nearly always a better expression of the stress or capability of equipment like generators. In most applications the voltage is fairly constant, so it's really similar to a rms current limit. Suppose you connect just a big capacitor to the output of your friends generator, it won't consume any power but the generator still has to work hard, deliver voltage and current, get hot, burn gas, etc. No fair calling the manufacturer and complaining that the generator won't deliver any power to your capacitor, nothing could. They'll say tough, we gave you lots of VA.

PS: It is common for generators to specify a minimum power factor limit for your load. Most don't like reactive loads.
 
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DaveE said:
PS: It is common for generators to specify a minimum power factor limit for your load. Most don't like purely reactive loads.
Yes, that was one thing I found confusing many years ago. A 30 kVA generator with a plated PF of 0.8, my understanding being that PF was a feature of the load, not the source. It was explained as a minimum load PF where full output can be guaranteed.
 
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Guineafowl said:
It was explained as a minimum load PF where full output can be guaranteed.
Or not break things.
 
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DaveE said:
Or not break things.
That might explain why it was totally burnt out when my friend got it home from a large machinery auction. It had come over from Spain to Scotland, and someone had thoughtfully disconnected all the wires from the alternator terminal box.

It’s a reasonably good Pramac 30 kVA ‘silent’ type, with Mecc-Alte alternator unit, and was otherwise in good condition and bristling with circuit breakers and RCDs. I wondered how they managed to cook the windings in those circumstances. Running for too long in a hot country with too low a PF would do it, I suppose.

One of those “could you just have a quick look at my…” jobs that turned out to be very interesting, swapping in a new (and VERY heavy) alternator into an enclosed box.
 
From another angle: The 'extra' power dissipation associated with reactive currents is part of the reason that large industrial customers of Electric Utilities are typically (U.S.) charged for both real energy consumption and Power Factor. That extra heating will happen in a transformer secondary or generator output windings.
 

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