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22-Elec-A1 Circuits · May 2016

Question 1 of 6: Equivalent resistance and source loading

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

Notes on this paper

Reference texts: C. K. Alexander & M. N. O. Sadiku, Fundamentals of Electric Circuits (7th ed., McGraw-Hill) — series/parallel reduction, Thévenin’s theorem with dependent sources, maximum-power transfer, first-order RC transients, AC phasor mesh analysis, complex power / power factor, and Laplace-domain (s-domain) circuit analysis; W. H. Hayt, J. E. Kemmerly & S. M. Durbin, Engineering Circuit Analysis (9th ed.) — companion treatment of the second-order source-driven RLC network and the initial-condition models used in Q6.

Closed-book national examination, 3 hours, six questions of equal value; any five constitute a complete paper. All six are solved here. A Laplace-transform table and a star–delta conversion table are supplied on the last two pages of the exam. Phasor magnitudes are quoted as magnitude $\angle$ angle with angles in degrees; a common cosine time reference is used, and the source marked rms in Q5 is treated as rms.

Question 1: Equivalent resistance and source loading [10 + (5+5)]

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. A $6\,\Omega$ resistor is connected directly across A–B (branch current $I_2$). A second branch leaves A through $8\,\Omega$ (current $I_1$) to node C, where a $20\,\Omega$ resistor and the unknown $R$ are connected in parallel between C and node D; from D a $10\,\Omega$ resistor returns to B. The specified terminal resistance is $R_{AB}=5\,\Omega$.

Find. (a) $R$ such that $R_{AB}=5\,\Omega$; (b) with $10\text{ V}$ across A–B, the current $I_R$ through $R$ and the total power delivered.

[Figure not reproduced: Figure 1 — redrawn. The $6\,\Omega$ is directly across A–B; the outer branch is $8\,\Omega$ in series with the parallel pair $20\,\Omega\,\|\,R$ (nodes C–D) in series with $10\,\Omega$. See the official exam paper.]

Approach. Reduce the outer branch to a single resistance in terms of $R$, set the parallel combination with the $6\,\Omega$ equal to $5\,\Omega$, solve for $R$; then re-energise with $10\text{ V}$ and use current division.

  1. Combine the parallel pair. The $20\,\Omega$ and $R$ share nodes C and D, so $$R_{CD}=\frac{20R}{20+R}.$$
  2. Series resistance of the outer branch. Adding the $8\,\Omega$ and $10\,\Omega$ in series, $$R_{\text{branch}} = 8 + \frac{20R}{20+R} + 10 = 18 + \frac{20R}{20+R}.$$
  3. Impose the terminal condition. This branch is in parallel with the $6\,\Omega$: $$R_{AB}= \frac{6\,R_{\text{branch}}}{6+R_{\text{branch}}}=5.$$ Solving, $6R_{\text{branch}} = 5(6+R_{\text{branch}})\Rightarrow R_{\text{branch}}=30\,\Omega.$
  4. Back out $R$. Then $18 + \dfrac{20R}{20+R}=30\Rightarrow \dfrac{20R}{20+R}=12\Rightarrow 20R = 12(20+R)\Rightarrow 8R=240.$ $$\boxed{R = 30\,\Omega}$$ As a check, $20\,\|\,30 = 12\,\Omega$, branch $=8+12+10=30\,\Omega$, and $6\,\|\,30 = 5\,\Omega.$ ✓
  5. (b) Total current from the $10\text{ V}$ source. With $R_{AB}=5\,\Omega$, $$I_{\text{total}}=\frac{10}{5}=2\text{ A}.$$ The current splits between the $6\,\Omega$ ($I_2=10/6=1.667\text{ A}$) and the $30\,\Omega$ outer branch ($I_1=10/30=0.333\text{ A}$); $1.667+0.333=2\text{ A}$ ✓.
  6. Current through $R$ by current division. $I_1=0.333\text{ A}$ reaches node C and develops $$V_{CD}=I_1\,(20\,\|\,R)=0.333\times12 = 4\text{ V},\qquad I_R=\frac{V_{CD}}{R}=\frac{4}{30}.$$ $$\boxed{I_R = 0.133\text{ A}=133.3\text{ mA}}$$ (The $20\,\Omega$ carries the remaining $4/20=0.200\text{ A}$; $0.133+0.200=0.333\text{ A}$ ✓.)
  7. Power supplied by the source. $$P = V\,I_{\text{total}} = 10\times 2 = \boxed{20\text{ W}}.$$
QuantityValue
Unknown resistance $R$$30\,\Omega$
Current through $R$, $I_R$$0.133\text{ A}$
Total source current $I_{\text{total}}$$2\text{ A}$
Power supplied by $10\text{ V}$ source$20\text{ W}$
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