The Junction Rectifier — Question 4

Section 41-8 · Physics pages 6938–6939

Question 4 An ideal half-wave rectifier has distinct mean and rms outputs A sinusoidal source vs = Vm sin θ drives an ideal diode and resistive load R. The output is vo = Vm sin θ for 0 < θ < π and zero for π < θ < 2π. θ vo π 2π Schematic; labels, not drawing lengths, specify the data. (a) Derive the mean and rms output voltages by integrating over a complete period. (b) Find the ratio of dc-component power to total load power and evaluate both voltages for Vm = 12.0 V.
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Question 4 - Solution An ideal half-wave rectifier has distinct mean and rms outputs θ vo π 2π (a) Method and calculation Vdc = 1 2π ∫π 0 Vm sin θ dθ = Vm/π . Vrms = √ 1 2π ∫π 0 V 2 m sin2 θ dθ = Vm/2 . (b) Interpretation and further calculation Pdc Pload = V 2 dc/R V 2 rms/R = 4/π2 = .4053 . Vdc = 3.820 V, Vrms = 6.00 V . Physical check The remaining load power is carried by the ac ripple component. This ratio is not the energy efficiency of an ideal lossless diode.

Question 4

An ideal half-wave rectifier has distinct mean and rms outputs

A sinusoidal source vs=Vmsin⁡θv_s=V_m\sin\theta drives an ideal diode and resistive load R. The output is vo=Vmsin⁡θv_o=V_m\sin\theta for 0<θ<π0<\theta<\pi and zero for π<θ<2π\pi<\theta<2\pi.

Diagram shown in the original SVG worksheet.

  1. Derive the mean and rms output voltages by integrating over a complete period.

  2. Find the ratio of dc-component power to total load power and evaluate both voltages for Vm=12.0VV_m=12.0\,\mathrm V.

Question 4 - Solution

An ideal half-wave rectifier has distinct mean and rms outputs

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Vdc=12π∫0πVmsin⁡θdθ=Vm/π.\boxed{V_{\mathrm{dc}}=\frac1{2\pi}\int_0^\pi V_m\sin\theta\,d\theta=V_m/\pi}.Vrms=12π∫0πVm2sin⁡2θdθ=Vm/2.\boxed{V_{\mathrm{rms}}=\sqrt{\frac1{2\pi}\int_0^\pi V_m^2\sin^2\theta\,d\theta}=V_m/2}.

(b) Interpretation and further calculation

PdcPload=Vdc2/RVrms2/R=4/π2=.4053.\boxed{\frac{P_{\mathrm{dc}}}{P_{\mathrm{load}}}=\frac{V_{\mathrm{dc}}^2/R}{V_{\mathrm{rms}}^2/R}=4/\pi^2=.4053}.Vdc=3.820V,Vrms=6.00V.\boxed{V_{\mathrm{dc}}=3.820\,\mathrm V,\quad V_{\mathrm{rms}}=6.00\,\mathrm V}.

Physical check

The remaining load power is carried by the ac ripple component. This ratio is not the energy efficiency of an ideal lossless diode.