The Junction Rectifier — Question 5

Section 41-8 · Physics pages 6940–6941

Question 5 Full-wave rectification doubles the ripple frequency An ideal bridge and resistive load give vo = Vm| sin ωt|. The source frequency is f, and there is no smoothing capacitor. ωt vo π 2π Schematic; labels, not drawing lengths, specify the data. (a) Derive average and rms output voltage. (b) Find the ripple frequency and the rms ripple factor r = √ V 2 rms −V 2 dc/Vdc.
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Question 5 - Solution Full-wave rectification doubles the ripple frequency ωt vo π 2π (a) Method and calculation Vdc = 1 π ∫π 0 Vm sin θ dθ = 2Vm/π . Vrms = Vm/ √ 2 . (b) Interpretation and further calculation vo(t + π/ω) = vo(t) ⇒fr = 2f . r = √ π2/8 −1 = .4834 . Physical check Both half cycles feed the load with the same polarity. The rms voltage is unchanged by taking the absolute value because its square is unchanged.

Question 5

Full-wave rectification doubles the ripple frequency

An ideal bridge and resistive load give vo=Vm|sin⁡ωt|v_o=V_m|\sin\omega t|. The source frequency is f, and there is no smoothing capacitor.

Diagram shown in the original SVG worksheet.

  1. Derive average and rms output voltage.

  2. Find the ripple frequency and the rms ripple factor r=Vrms2−Vdc2/Vdcr=\sqrt{V_{\mathrm{rms}}^2-V_{\mathrm{dc}}^2}/V_{\mathrm{dc}}.

Question 5 - Solution

Full-wave rectification doubles the ripple frequency

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Vdc=1π∫0πVmsin⁡θdθ=2Vm/π.\boxed{V_{\mathrm{dc}}=\frac1\pi\int_0^\pi V_m\sin\theta\,d\theta=2V_m/\pi}.Vrms=Vm/2.\boxed{V_{\mathrm{rms}}=V_m/\sqrt2}.

(b) Interpretation and further calculation

vo(t+π/ω)=vo(t)⇒fr=2f.v_o(t+\pi/\omega)=v_o(t)\Rightarrow\boxed{f_r=2f}.r=π2/8−1=.4834.\boxed{r=\sqrt{\pi^2/8-1}=.4834}.

Physical check

Both half cycles feed the load with the same polarity. The rms voltage is unchanged by taking the absolute value because its square is unchanged.