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22-Elec-A1 Circuits · December 2014

Question 5 of 6: AC Thévenin equivalent and maximum power transfer

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

Notes on this paper

Paper: National Examinations — 07-Elec-A1 Circuits, December 2014. Closed-book, 3-hour paper; a Laplace-transform table and Y–Δ formulas are supplied in the appendix. Six questions of equal value; any five constitute a complete paper. Full worked solutions to all six questions are given below so the set can be used for study regardless of which five a candidate chose.

Reference texts: C. K. Alexander & M. N. O. Sadiku, Fundamentals of Electric Circuits (7th ed., McGraw-Hill) — series/parallel reduction and the Wheatstone bridge, mesh/supermesh and nodal analysis, first-order transients, AC steady-state, Thévenin’s theorem and maximum-power transfer, and Laplace-domain circuit analysis; W. H. Hayt, J. E. Kemmerly & S. M. Durbin, Engineering Circuit Analysis (9th ed.) — companion treatment of the s-domain and initial-condition source models.

each network below is redrawn element-by-element from the original drawing. The Wheatstone bridge of Q1 is shown in the equivalent rectangular form (electrically identical to the diamond on the paper). Every reference node, mesh direction and source polarity used is stated with its solution so a reader can reproduce every sign. Phasor answers are quoted in magnitude∡angle form with angles in degrees; the source of Q5 is rms.

Question 5: AC Thévenin equivalent and maximum power transfer [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. An rms source $V_s=100\angle30^{\circ}\text{ V}$ feeds two series ladders that meet the open terminals A and B:

BranchTo terminal A (left)To terminal B (right)
from + rail$10\,\Omega$ then $-j5\,\Omega$$4\,\Omega$ then $j8\,\Omega$
from $-$ rail$5\,\Omega$$6\,\Omega$

Find. The Thévenin voltage $V_{th}$ and impedance $Z_{th}$ at A–B; the load $Z_{Load}$ for maximum power; and that maximum power.

[Figure not reproduced: Figure-5 (redrawn). Terminal A is the mid-point of the left ladder ($10\,\Omega,-j5\,\Omega$ above; $5\,\Omega$ below) and B the mid-point of the right ladder ($4\,\Omega,j8\,\Omega$ above; $6\,\Omega$ below). Each ladder is a voltage divider across the source. See the official exam paper.]

Approach. Each terminal is the tap of a voltage divider, so $V_{th}=V_A-V_B$ (open circuit). For $Z_{th}$, short the source (the two rails merge) and combine the parallel pairs seen from A and from B, in series. Maximum power to a complex load requires $Z_{Load}=Z_{th}^{*}$, and $P_{max}=|V_{th}|^2/(4R_{th})$ for rms phasors.

  1. Open-circuit node voltages. With A and B open, each ladder is an undivided series divider from the $+$ rail to the $-$ rail. Taking the $-$ rail as reference and $V_s$ on the $+$ rail, the tap voltages (across the lower resistor of each ladder) are $$V_A=V_s\,\frac{5}{10-j5+5}=V_s\,\frac{5}{15-j5}=31.62\angle48.43^{\circ}\ \text{V},$$ $$V_B=V_s\,\frac{6}{4+j8+6}=V_s\,\frac{6}{10+j8}=46.85\angle{-8.66^{\circ}}\ \text{V}.$$
  2. Thévenin voltage (i). $$V_{th}=V_A-V_B=31.62\angle48.43^{\circ}-46.85\angle{-8.66^{\circ}}=\boxed{39.82\angle129.5^{\circ}\ \text{V (rms)}}.$$
  3. Thévenin impedance (i). Kill the source (short the two rails together). Looking into A, the upper arm $(10-j5)$ parallels the lower $5\,\Omega$; looking into B, the upper $(4+j8)$ parallels the lower $6\,\Omega$; the two results are in series between A and B: $$Z_{th}=\big[(10-j5)\|5\big]+\big[(4+j8)\|6\big]=(3.50-j0.50)+(3.80+j1.76),$$ $$Z_{th}=\boxed{7.30+j1.26\ \Omega}=7.41\angle9.76^{\circ}\ \Omega.$$
  4. Load for maximum power (ii). Conjugate match: $$Z_{Load}=Z_{th}^{*}=\boxed{7.30-j1.26\ \Omega}\;(=7.41\angle{-9.76^{\circ}}\ \Omega).$$
  5. Maximum power (iii). With the match, the load resistance equals $R_{th}=7.30\,\Omega$ and the reactances cancel; for rms phasors $$P_{max}=\frac{|V_{th}|^{2}}{4R_{th}}=\frac{39.82^{2}}{4(7.30)}=\boxed{54.26\ \text{W}}.$$
QuantityResult
$V_{th}$$\boxed{39.82\angle129.5^{\circ}\ \text{V (rms)}}$
$Z_{th}$$\boxed{7.30+j1.26\ \Omega}$
$Z_{Load}=Z_{th}^{*}$$\boxed{7.30-j1.26\ \Omega}$
$P_{max}$$\boxed{54.26\ \text{W}}$