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22-Elec-A1 Circuits · May 2017

Question 1 of 6: Equivalent resistance, source current and a branch current

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 and Δ–Y reduction, mesh/nodal analysis with dependent sources, first-order transients, AC phasor analysis, Thévenin equivalents, maximum-power transfer and Laplace (s-domain) analysis; W. H. Hayt, J. E. Kemmerly & S. M. Durbin, Engineering Circuit Analysis (9th ed.) — companion treatment of super-mesh/super-node bookkeeping and the initial-condition source 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 written as magnitude $\angle$ angle with angles in degrees; a sine (peak) time reference is used in Q4 to match the source $100\sin377t$, and the sources marked rms in Q5 are treated as rms.

Question 1: Equivalent resistance, source current and a branch current [10 + 4 + 6]

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 $100\text{ V}$ source $E_s$ drives the terminal pair a–b. Reading Figure 1: the $5\,\Omega$ is in series from a to the whole top rail (one node, call it $T$). From $T$ three resistors drop to the network: $10\,\Omega$ to node $D$, $12\,\Omega$ to node $E$, and $20\,\Omega$ straight to b. A $6\,\Omega$ bridges $D$–$E$; $11\,\Omega$ joins $D$–b and $15\,\Omega$ joins $E$–b.

BranchValueBranchValue
a–$T$ (series)$5\,\Omega$$D$–$E$ (bridge)$6\,\Omega$
$T$–$D$$10\,\Omega$$D$–b$11\,\Omega$
$T$–$E$$12\,\Omega$$E$–b$15\,\Omega$
$T$–b$20\,\Omega$Source $E_s$$100\text{ V}$

Find. $R_{ab}$, then $I_s=E_s/R_{ab}$, then the current $I_1$ down the $20\,\Omega$ branch.

[Figure not reproduced: Figure 1 — redrawn. The entire top wire right of the $5\,\Omega$ is a single node $T$; the $6\,\Omega$ bridges the two inner columns, so the $T$–$D$–$E$–b block is a bridge that has no pure series/parallel reduction. See the official exam paper.]

Approach. The $D$–$E$–b sub-network is a $\Delta$; convert it to a Y so the remainder collapses by series/parallel, giving $R_{Tb}$ and hence $R_{ab}=5+R_{Tb}$; then $I_s=100/R_{ab}$ and $I_1=V_T/20$ with $V_T=100-5I_s$.

  1. Convert the $\Delta$ ($6,11,15$) on nodes $D,E,$b to a Y. With $\Sigma=6+11+15=32\,\Omega$, the Y arms at $D$, $E$ and b are $$R_D=\frac{6\cdot11}{32}=2.063\,\Omega,\quad R_E=\frac{6\cdot15}{32}=2.813\,\Omega,\quad R_b=\frac{11\cdot15}{32}=5.156\,\Omega.$$
  2. Add the series arms up each column. The Y centre now reaches $T$ through two parallel legs: $10+R_D=12.063\,\Omega$ and $12+R_E=14.813\,\Omega$.
  3. Parallel the two legs, then add $R_b$. $$\frac{12.063\cdot14.813}{12.063+14.813}=6.649\,\Omega,\qquad 6.649+R_b=6.649+5.156=11.806\,\Omega\ (T\text{ to }b\text{ via the Y}).$$
  4. Parallel that with the direct $20\,\Omega$ ($T$–b). $$R_{Tb}=\frac{11.806\cdot20}{11.806+20}=7.423\,\Omega.$$
  5. (a) Add the series $5\,\Omega$. $$\boxed{R_{ab}=5+7.423=12.42\,\Omega.}$$
  6. (b) Source current. $$\boxed{I_s=\frac{E_s}{R_{ab}}=\frac{100}{12.42}=8.05\text{ A}.}$$
  7. (c) Current in the $20\,\Omega$. The top node sits at $V_T=100-5I_s=100-5(8.05)=59.75\text{ V}$ above b, and the $20\,\Omega$ runs straight from $T$ to b, so $$\boxed{I_1=\frac{V_T}{20}=\frac{59.75}{20}=2.99\text{ A}.}$$
QuantityValue
Equivalent resistance $R_{ab}$$12.42\,\Omega$
Source current $I_s$$8.05\text{ A}$
Current in $20\,\Omega$, $I_1$$2.99\text{ A}$
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