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Physics · Ch 4 — Electromagnetic Induction and Alternating Current

Introduction of Power in AC Circuits

4.8.1

Introduction of Power in AC Circuits

The power of a circuit is the rate at which it consumes electric energy, given at any instant by the product of the instantaneous voltage and current. With v=Vmsin⁡ωtv=V_m\sin\omega t and, allowing for a general phase angle ϕ\phi between voltage and current (as in a series RLC circuit), i=Imsin⁡(ωt+ϕ)i=I_m\sin(\omega t+\phi), the instantaneous power is

P=vi=VmImsin⁡ωtsin⁡(ωt+ϕ)P = vi = V_mI_m\sin\omega t\sin(\omega t+\phi)

Expanding sin⁡(ωt+ϕ)=sin⁡ωtcos⁡ϕ+cos⁡ωtsin⁡ϕ\sin(\omega t+\phi)=\sin\omega t\cos\phi+\cos\omega t\sin\phi and multiplying out gives

P=VmIm[cos⁡ϕsin⁡2ωt+sin⁡ωtcos⁡ωtsin⁡ϕ](4.54)P = V_mI_m\left[\cos\phi\sin^2\omega t + \sin\omega t\cos\omega t\sin\phi\right] \qquad (4.54)

Averaging this over a complete cycle, and using the standard time-averages ⟨sin⁡2ωt⟩=12\langle\sin^2\omega t\rangle=\tfrac12 and ⟨sin⁡ωtcos⁡ωt⟩=0\langle\sin\omega t\cos\omega t\rangle=0, gives the average power

Pav=VmIm2cos⁡ϕ=Vm2⋅Im2cos⁡ϕP_{av} = \dfrac{V_mI_m}{2}\cos\phi = \dfrac{V_m}{\sqrt2}\cdot\dfrac{I_m}{\sqrt2}\cos\phi

or, in terms of RMS values,

Pav=VRMSIRMScos⁡ϕ(4.55)P_{av} = V_{RMS}I_{RMS}\cos\phi \qquad (4.55) …