22-Elec-A1 Circuits · December 2018
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Reference texts: C. K. Alexander & M. N. O. Sadiku, Fundamentals of Electric Circuits (7th ed., McGraw-Hill) — series/parallel and Δ–Y reduction, superposition, node analysis with dependent sources, first-order RC transients, AC phasor/node analysis, Thévenin equivalents and maximum-power transfer, and Laplace (s-domain) analysis of second-order circuits; W. H. Hayt, J. E. Kemmerly & S. M. Durbin, Engineering Circuit Analysis (9th ed.) — companion treatment of 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 as a study resource. 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; because $e$ and $i$ in Q5 are written as $40\sqrt2\cos$ and $5\sqrt2\cos$ (peak $=\sqrt2\times$rms), rms phasors $\mathbf E=40\angle30^\circ$ V and $\mathbf I=5\angle0^\circ$ A are used so the computed power is in watts directly.
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. $e=40\sqrt2\cos(\omega t+30^\circ)$ (rms phasor $\mathbf E=40\angle30^\circ$ V) drives a source node through $C=0.00133\text{ F}$ to node 1; a $3\,\Omega$ ties node 1 to ground; a series $8\,\Omega+L$ ($L=0.016\text{ H}$) links nodes 1 and 2; a $10\,\Omega$ ties node 2 to ground; and $i=5\sqrt2\cos\omega t$ (rms phasor $\mathbf I=5\angle0^\circ$ A) injects into node 2. At $f=60\text{ Hz}$, $\omega=2\pi(60)=377\text{ rad/s}$.
| Quantity | Value | Impedance | Value |
|---|---|---|---|
| $\omega$ | $377\text{ rad/s}$ | $Z_C=1/(j\omega C)$ | $-j1.99\,\Omega\;(\approx-j2)$ |
| $L$ | $0.016\text{ H}$ | $Z_L=j\omega L$ | $+j6.03\,\Omega\;(\approx+j6)$ |
| Branch 1–2 | $8\,\Omega+Z_L$ | $Z_b$ | $8+j6.03\,\Omega$ |
Find. the node equations, the phasor node voltages $\mathbf V_1,\mathbf V_2$, and the real power delivered by $e$.
Approach. Convert every element to an admittance, write KCL at nodes 1 and 2 (the source node voltage equals $\mathbf E$), solve the $2\times2$ complex system, then compute $\mathbf S=\mathbf E\,\mathbf I_e^{*}$ for the source.
| Quantity | Result |
|---|---|
| Node voltage $\mathbf V_1$ | $29.4\angle62.8^\circ\text{ V}$ |
| Node voltage $\mathbf V_2$ | $40.9\angle28.0^\circ\text{ V}$ |
| Source current $\mathbf I_e$ | $11.08\angle73.8^\circ\text{ A}$ |
| Real power supplied by $e$ | $319.7\text{ W}$ |