The Junction Rectifier — Question 6

Section 41-8 · Physics pages 6942–6943

Question 6 Finite bridge drops reduce the conduction interval A bridge rectifier has two conducting diodes in each path, each modeled by fixed drop Vf. With resistive load and sinusoidal source, vo = max(Vm| sin θ| −2Vf, 0). Let Vm = 10.0 V and Vf = .700 V. θ vo Schematic; labels, not drawing lengths, specify the data. (a) Find the conduction angle during each rectified half cycle. (b) Derive and evaluate the average output voltage.
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Question 6 - Solution Finite bridge drops reduce the conduction interval θ vo (a) Method and calculation θ0 = sin−1(2Vf/Vm) = sin−1(.14) = .14046 rad. ∆θ = π −2θ0 = 2.86067 rad = 163.9◦. (b) Interpretation and further calculation Vdc = 1 π ∫π−θ0 θ0 (Vm sin θ −2Vf)dθ. Vdc = 2Vm cos θ0 −2Vf(π −2θ0) π = 5.029 V . Physical check Subtracting 2Vf from the ideal mean would incorrectly include negative output near each zero crossing. The clipped intervals must be removed from the integral.

Question 6

Finite bridge drops reduce the conduction interval

A bridge rectifier has two conducting diodes in each path, each modeled by fixed drop VfV_f. With resistive load and sinusoidal source, vo=max⁡(Vm|sin⁡θ|−2Vf,0)v_o=\max(V_m|\sin\theta|-2V_f,0). Let Vm=10.0VV_m=10.0\,\mathrm V and Vf=.700VV_f=.700\,\mathrm V.

Diagram shown in the original SVG worksheet.

  1. Find the conduction angle during each rectified half cycle.

  2. Derive and evaluate the average output voltage.

Question 6 - Solution

Finite bridge drops reduce the conduction interval

Diagram shown in the original SVG worksheet.

(a) Method and calculation

θ0=sin⁡−1(2Vf/Vm)=sin⁡−1(.14)=.14046rad.\theta_0=\sin^{-1}(2V_f/V_m)=\sin^{-1}(.14)=.14046\,\mathrm{rad}.Δθ=π−2θ0=2.86067rad=163.9∘.\boxed{\Delta\theta=\pi-2\theta_0=2.86067\,\mathrm{rad}=163.9^\circ}.

(b) Interpretation and further calculation

Vdc=1π∫θ0π−θ0(Vmsin⁡θ−2Vf)dθ.V_{\mathrm{dc}}=\frac1\pi\int_{\theta_0}^{\pi-\theta_0}(V_m\sin\theta-2V_f)d\theta.Vdc=2Vmcos⁡θ0−2Vf(π−2θ0)π=5.029V.\boxed{V_{\mathrm{dc}}=\frac{2V_m\cos\theta_0-2V_f(\pi-2\theta_0)}{\pi}=5.029\,\mathrm V}.

Physical check

Subtracting 2Vf from the ideal mean would incorrectly include negative output near each zero crossing. The clipped intervals must be removed from the integral.