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22-Elec-A5 Electronics · May 2016

Question 3 of 5: Ideal-Diode Resistor Network

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

Notes on this paper

National Exam — 07-Elec-A5 Electronics — May 2016. Closed-book; non-communicating calculator permitted; three hours. Five questions, 20 marks each — all five constitute a complete paper, so every question is solved below. Op-amps are ideal with supply rails of ±15 V unless a question states otherwise.

Reference texts (22-Elec-A5 Electronics): A. S. Sedra & K. C. Smith, Microelectronic Circuits, 7th/8th ed. (Oxford) — diodes (Ch. 4), MOSFETs and biasing (Ch. 5/7), op-amp circuits (Ch. 2), signal generators / wave-shaping (Ch. 17), MOS logic inverters (Ch. 14); R. C. Jaeger & T. N. Blalock, Microelectronic Circuit Design (McGraw-Hill).

Check / figure note: every schematic below was redrawn from the printed figures of the paper. Where the paper omits a numeric supply (Q1), the transfer curve is drawn to scale for an illustrative VDD = 5 V and the symbolic result is stated alongside.

Question 3: Ideal-Diode Resistor Network (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 (Question 3)
ElementValueConnection
R110 kΩ+10 V to node A (carries I1)
R210 kΩnode VL to −20 V (I2)
R310 kΩnode VB to −10 V (I3)
D10.6 Vanode A, cathode VL
D20.6 Vanode A, cathode VB
D30.6 Vanode ground, cathode VB

Find. the branch currents $I_1,\,I_2,\,I_3$.

+10 VR1D1D2D3R2-20 VR3-10 VI1I2I3
Figure 3. Diode network: node A sits below R1; D1/D2 steer from A, D3 connects ground to node VB.

Approach. Ideal diodes are switches with a fixed 0.6 V drop when on; assume an on/off state, solve the resulting linear node equations, then confirm every “on” diode carries forward current and every “off” diode is reverse-biased.

  1. Trial state. Try D1 on, D3 on, D2 off. Then D3 pins $v_B=0-0.6=-0.6$ V and D1 gives $v_L=v_A-0.6$.
  2. Node A (with D2 off). All of I1 leaves A through D1 into VL and down R2, so $I_1=I_2$. Writing both currents: $\dfrac{10-v_A}{R}=\dfrac{v_L+20}{R}$ with $v_L=v_A-0.6$ $$\Rightarrow 10-v_A=v_A-0.6+20\Rightarrow \boxed{v_A=-4.7\ \text{V}},\ v_L=-5.3\ \text{V}.$$
  3. Currents I1, I2. $$I_1=\frac{10-(-4.7)}{10\text{ k}}=1.47\ \text{mA},\qquad I_2=\frac{-5.3+20}{10\text{ k}}=1.47\ \text{mA}.$$ As required $I_1=I_2$ (series through the conducting D1).
  4. Node VB and I3. With $v_B=-0.6$ V, the current down R3 is $$I_3=\frac{-0.6-(-10)}{10\text{ k}}=\boxed{0.94\ \text{mA}}$$ supplied entirely by D3 from ground ($I_{D3}=0.94$ mA > 0, so D3 is legitimately on).
  5. Consistency of D2 (off). $v_A-v_B=-4.7-(-0.6) =-4.1$ V < 0.6 V, so D2 is reverse-biased — the assumed state is self-consistent, and $I_1=1.47,\;I_2=1.47,\;I_3=0.94$ mA is the unique solution.
Question 3 — branch currents
CurrentPathValue
$I_1$+10 V → R1 → A1.47 mA
$I_2$VL → R2 → −20 V1.47 mA
$I_3$VB → R3 → −10 V0.94 mA