Instantaneous Power in Nonsinusoidal Circuits

Instantaneous power $p(t)=u(t)i(t)$ remains exact for arbitrary waveforms, while the familiar sinusoidal power triangle does not. Average power and RMS define a useful orthogonal current projection, but reactive-power decompositions are model-dependent.

The product

p(t)=u(t)i(t)p(t)=u(t)i(t)

is instantaneous terminal power for any waveforms. Its interval average

P=1T∫0Tu(t)i(t) dtP=\frac{1}{T}\int_0^T u(t)i(t)\,dt

is net active power. These statements survive distortion, harmonics, switching, and nonperiodic observation windows. What does not survive unchanged is the unique sinusoidal interpretation S=P+jQS=P+jQ.

RMS and apparent power #

Over the same interval,

U=1T∫0Tu2(t) dt,I=1T∫0Ti2(t) dt.U=\sqrt{\frac1T\int_0^T u^2(t)\,dt},\qquad I=\sqrt{\frac1T\int_0^T i^2(t)\,dt}.

S=UIS=UI is apparent power and P/SP/S is total power factor. Harmonic distortion can lower that ratio even when the fundamental voltage and current have no phase displacement.

Orthogonal current projection #

Treat waveforms as vectors with inner product

⟨x,y⟩=1T∫0Tx(t)y(t) dt.\langle x,y\rangle=\frac1T\int_0^T x(t)y(t)\,dt.

Project current onto voltage:

ia(t)=PU2u(t),ir(t)=i(t)−ia(t).i_a(t)=\frac{P}{U^2}u(t),\qquad i_r(t)=i(t)-i_a(t).

Then ⟨u,ir⟩=0\langle u,i_r\rangle=0. The projected current iai_a is the minimum-RMS current waveform that transfers the same average power for the given voltage, and its equivalent conductance is G=P/U2G=P/U^2.

The residual contains every current component that transfers zero net energy over the chosen interval: phase-shifted fundamental current, harmonic current orthogonal to the voltage, and possibly distortion unrelated to energy storage.

Spectral view #

For periodic waveforms in a linear system, average power is the sum of same-frequency voltage-current contributions; different harmonics are orthogonal over an integer number of periods. A window that does not contain coherent periods introduces leakage into both spectral and time-domain averages.

Always state the averaging interval and power definition. Competing nonsinusoidal reactive-power theories answer different engineering questions and should not be mixed by notation alone.

For measured waveforms, align voltage and current channels before multiplying them. A relative timing error creates an apparent phase shift and therefore biases both average power and any residual-current decomposition.

Sources

  1. paperTheoretical Aspects and Methods of Parameters Identification of Devices of the Electric Traction System: Method of Instantaneous Powers; Parallel Connection of Elementspdfnotes

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