Alternating Current — Question 2

Section 31-5 · Physics pages 5054–5055

Question 2 Zero mean voltage can deliver a nonzero mean heating rate A resistor R carries i(t) = Ip sin ωt. Average over one complete period. ωt i/Ip Schematic; labels, not drawing lengths, specify the data. (a) Derive mean current, rms current, and mean power directly from the integrals. (b) Find energy dissipated over n complete cycles.
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Question 2 - Solution Zero mean voltage can deliver a nonzero mean heating rate ωt i/Ip (a) Method and calculation ⟨i⟩= Ip 2π ∫2π 0 sin θ dθ = 0. I2 rms = I2 p 2π ∫2π 0 sin2 θ dθ = I2 p/2 . (b) Interpretation and further calculation ⟨P⟩= R⟨i2⟩= RI2 p/2. Hn = ⟨P⟩nT = πnRI2 p/ω . Physical check Heating depends on squared current, so opposite half-cycles both contribute positively.

Question 2

Zero mean voltage can deliver a nonzero mean heating rate

A resistor R carries i(t)=Ipsin⁡ωti(t)=I_p\sin\omega t. Average over one complete period.

Diagram shown in the original SVG worksheet.

  1. Derive mean current, rms current, and mean power directly from the integrals.

  2. Find energy dissipated over n complete cycles.

Question 2 - Solution

Zero mean voltage can deliver a nonzero mean heating rate

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨i⟩=Ip2π∫02πsin⁡θdθ=0.\langle i\rangle=\frac{I_p}{2\pi}\int_0^{2\pi}\sin\theta\,d\theta=0.Irms2=Ip22π∫02πsin⁡2θdθ=Ip2/2.\boxed{I_{\mathrm{rms}}^2=\frac{I_p^2}{2\pi}\int_0^{2\pi}\sin^2\theta\,d\theta=I_p^2/2}.

(b) Interpretation and further calculation

⟨P⟩=R⟨i2⟩=RIp2/2.\langle P\rangle=R\langle i^2\rangle=RI_p^2/2.Hn=⟨P⟩nT=πnRIp2/ω.\boxed{H_n=\langle P\rangle nT=\pi n RI_p^2/\omega}.

Physical check

Heating depends on squared current, so opposite half-cycles both contribute positively.