Alternating Current — Question 6

Section 31-5 · Physics pages 5062–5063

Question 6 Half-wave rectification changes both mean and rms in different proportions An ideal rectifier passes Vp sin ωt during the positive half-cycle and outputs zero during the negative half-cycle. Ignore diode drop. ωt v Schematic; labels, not drawing lengths, specify the data. (a) Find the cycle mean and rms output voltage. (b) Find the AC-only rms ripple after subtracting the mean.
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Question 6 - Solution Half-wave rectification changes both mean and rms in different proportions ωt v (a) Method and calculation ¯v = Vp 2π ∫π 0 sin θdθ = Vp/π. V 2 rms = V 2 p 2π ∫π 0 sin2 θdθ = V 2 p /4 . (b) Interpretation and further calculation V 2 ripple,rms = ⟨(v −¯v)2⟩= V 2 rms −¯v2. Vripple,rms = Vp √ 1/4 −1/π2 . Physical check Removing the DC mean reduces rms ripple but does not alter the definition of total rms.

Question 6

Half-wave rectification changes both mean and rms in different proportions

An ideal rectifier passes Vpsin⁡ωtV_p\sin\omega t during the positive half-cycle and outputs zero during the negative half-cycle. Ignore diode drop.

Diagram shown in the original SVG worksheet.

  1. Find the cycle mean and rms output voltage.

  2. Find the AC-only rms ripple after subtracting the mean.

Question 6 - Solution

Half-wave rectification changes both mean and rms in different proportions

Diagram shown in the original SVG worksheet.

(a) Method and calculation

v‾=Vp2π∫0πsin⁡θdθ=Vp/π.\bar v=\frac{V_p}{2\pi}\int_0^\pi\sin\theta d\theta=V_p/\pi.Vrms2=Vp22π∫0πsin⁡2θdθ=Vp2/4.\boxed{V_{\mathrm{rms}}^2=\frac{V_p^2}{2\pi}\int_0^\pi\sin^2\theta d\theta=V_p^2/4}.

(b) Interpretation and further calculation

Vripple,rms2=⟨(v−v‾)2⟩=Vrms2−v‾2.V_{{\mathrm{ripple}},\mathrm{rms}}^2=\langle(v-\bar v)^2\rangle=V_{\mathrm{rms}}^2-\bar v^2.Vripple,rms=Vp1/4−1/π2.\boxed{V_{{\mathrm{ripple}},\mathrm{rms}}=V_p\sqrt{1/4-1/\pi^2}}.

Physical check

Removing the DC mean reduces rms ripple but does not alter the definition of total rms.