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22-Elec-A1 Circuits · December 2018

Question 5 of 6: AC node-voltage analysis and source power

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, 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 5: AC node-voltage analysis and source power [8 + 6 + 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.

+−+−e = 40√2 cos(ωt+30°)0.00133 F13Ω8Ω0.016 H210Ωi = 5√2 cosωt
Figure‑5 — 60 Hz ac network. Source e sets the left node; the series 8Ω+0.016 H links nodes 1 and 2; current source i injects into node 2. Reference is the bottom rail.

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 $f=60\text{ Hz}$, $\omega=2\pi(60)=377\text{ rad/s}$.

QuantityValueImpedanceValue
$\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.

  1. (a) Node equations. With the bottom rail as reference and the source node held at $\mathbf E$, KCL at nodes 1 and 2 reads $$\frac{\mathbf V_1-\mathbf E}{Z_C}+\frac{\mathbf V_1}{3}+\frac{\mathbf V_1-\mathbf V_2}{Z_b}=0,\qquad \frac{\mathbf V_2-\mathbf V_1}{Z_b}+\frac{\mathbf V_2}{10}=\mathbf I,$$ with $Z_C=-j1.99\,\Omega$, $Z_b=8+j6.03\,\Omega$, $\mathbf E=40\angle30^\circ$ V and $\mathbf I=5\angle0^\circ$ A.
  2. Admittance form. Using $Y_C=1/Z_C=j0.501\text{ S}$ and $Y_b=1/Z_b=0.0797-j0.0601\text{ S}$: $$(Y_C+\tfrac13+Y_b)\mathbf V_1-Y_b\mathbf V_2=\mathbf E\,Y_C,\qquad -Y_b\mathbf V_1+(Y_b+\tfrac1{10})\mathbf V_2=\mathbf I.$$
  3. (b) Solve the node voltages. Solving the $2\times2$ complex system: $$\boxed{\mathbf V_1=29.4\angle62.8^\circ\text{ V},\qquad \mathbf V_2=40.9\angle28.0^\circ\text{ V}.}$$
  4. Source current. All of the source current flows through $C$ into node 1: $$\mathbf I_e=\frac{\mathbf E-\mathbf V_1}{Z_C}=11.08\angle73.8^\circ\text{ A (rms)}.$$
  5. Power supplied by $e$. The complex power delivered is $$\mathbf S=\mathbf E\,\mathbf I_e^{*}=(40\angle30^\circ)(11.08\angle{-73.8^\circ})=319.7-j306.8\text{ VA},$$ so the real power supplied is $$\boxed{P_e=\operatorname{Re}\{\mathbf S\}=319.7\text{ W}}$$ (with $306.8\text{ VAR}$ delivered capacitively/leading).
QuantityResult
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}$