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22-Elec-A5 Electronics · May 2013

Question 5 of 6: Bridge Rectifier with a Failed Diode

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. National Exams, May 2013 — 07-Elec-A5 Electronics. Three hours, closed book; one approved Casio or Sharp calculator permitted. Six questions are printed, each worth 20 marks, and five constitute a complete paper — all six are solved below as a study resource. Op-amps are ideal with ±15 V supplies unless stated otherwise.

Reference texts. A. S. Sedra & K. C. Smith, Microelectronic Circuits, 8th ed. (Oxford): Ch. 5–7 (MOSFET and BJT amplifiers, common-emitter and common-gate stages), Ch. 4 (diode limiters, clamps and rectifiers), Ch. 13–14 (CMOS/NMOS inverter VTC and noise margins), and Ch. 2 (op-amp precision rectifiers and slew rate).

Question 5: Bridge Rectifier with a Failed Diode (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given.

Given data
QuantityValueQuantityValue
Input1 kHz triangle, ±10 VPeriod T1 ms
RC5 msDiode drop0 (ideal)
D1open (destroyed)Rectifierbridge → half-wave

Find. The output waveform, $V_p$, $V_r$, the average output, and the diode conduction time $t_{on}$.

[Figure not reproduced: Q5 circuit (redrawn): full-wave bridge with the left node grounded and the output taken from the right node into the C||R filter. D1 (red X) is open. The surviving pair D2, D3 conducts only on the POSITIVE half of v_s, so the stage is now a half-wave rectifier. See the official exam paper.]

Approach. Establish that losing $D_1$ turns the bridge into a half-wave rectifier, then apply the standard peak / ripple / average / conduction-angle relations for a capacitor-filtered rectifier, using the triangular slope for the conduction interval.

  1. Effect of the open diode. In the bridge, $D_1$ conducts (with $D_4$) on the negative half of $v_s$. With $D_1$ open that half can no longer conduct, while the surviving pair $D_2,D_3$ still conducts on the positive half. The stage is now a half-wave rectifier: $C$ recharges only once per input period, so the ripple frequency drops from 2 kHz to $$f=1\ \text{kHz},\qquad T=1\ \text{ms}.$$
  2. (b) Peak voltage. The diodes are ideal (zero drop), so $C$ charges to the input peak: $$\boxed{V_p=10\ \text{V}}.$$
  3. (b) Ripple. Between charging pulses $C$ discharges through $R$ for one full period. The standard estimate $$V_r\approx\frac{V_p\,T}{RC}=\frac{10\times1\ \text{ms}}{5\ \text{ms}}=\boxed{2\ \text{V}}$$ (the exact exponential $V_p(1-e^{-T/RC})=1.81$ V is close, confirming the linear approximation).
  4. (c) Average output. The output rides between $V_p$ and $V_p-V_r$, so $$V_{o,avg}\approx V_p-\frac{V_r}{2}=10-1=\boxed{9\ \text{V}}.$$
  5. (d) Conduction interval. On the rising edge the triangle climbs at $|dv/dt|=20\ \text{V}/0.5\ \text{ms}=40\ \text{V}/\text{ms}$. The diodes conduct only while the input rises from $V_p-V_r$ back up to $V_p$, a climb of $V_r$: $$t_{on}\approx\frac{V_r}{|dv/dt|}=\frac{2\ \text{V}}{40\ \text{V}/\text{ms}}=0.05\ \text{ms}=\boxed{50\ \mu\text{s}}.$$
t (ms)v (V)12310-10Vp=10
Output v_o with D1 open (blue): the bridge acts as a HALF-wave rectifier, so C recharges only once per 1 ms period (positive peaks). Peak V_p=10 V, peak-to-peak ripple ~2 V, average ~9 V. Dashed grey = triangular input.
Q5 — results
QuantityValue
Rectificationhalf-wave (D1 open), f = 1 kHz
Peak Vp10 V
Ripple Vr≈ 2 V (exact 1.81 V)
Average Vo≈ 9 V
Conduction time ton≈ 50 µs