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22-Elec-A1 Circuits · May 2017

Question 2 of 6: Mesh analysis with a dependent source

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 2: Mesh analysis with a dependent source [8 + 8 + 4]

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. Four clockwise mesh currents $I_1,I_2,I_3,I_4$. A $2\text{ A}$ independent source is shared by meshes $1$ and $2$; a dependent source $4I_o$ (arrow up) is shared by meshes $1$ and $3$; $I_o$ is the current in the $1\,\Omega$ resistor (top of mesh $4$), drawn pointing left. Resistors: $5\,\Omega$ (only in mesh $1$), $4\,\Omega$ (mesh $2$), $3\,\Omega$ (mesh $3$), $6\,\Omega$ (shared by meshes $3$ and $4$), $1\,\Omega$ (mesh $4$); a $15\text{ V}$ source (+ up) closes mesh $4$.

Find. the four mesh currents and $P_{6\Omega}$.

[Figure not reproduced: Figure 2 — redrawn, all four mesh currents clockwise. The two current sources are internal branches, so the meshes they join are merged into one super-mesh for the KVL walk. Because $I_1$ links to both $I_2$ (via $2\text{ A}$) and $I_3$ (via $4I_o$), meshes $1$–$2$–$3$ form a . See the official exam paper.]

Approach. Take each current source as a mesh-current constraint, write one super-mesh KVL around the combined loop $1$–$2$–$3$ and one ordinary KVL for mesh $4$, express $I_o$ through $I_4$, then solve the $4\times4$ set; the $6\,\Omega$ carries $I_3-I_4$.

  1. (a) Source constraints. The $2\text{ A}$ source fixes the difference of the meshes on either side of it, and the dependent source fixes the other pair: $$I_2-I_1=2,\qquad I_3-I_1=4I_o.$$ The controlling current is the $1\,\Omega$ current $I_o$; drawn opposite to the clockwise $I_4$, so $$I_o=-I_4.$$
  2. (a) Super-mesh KVL (meshes 1–2–3). Walking the outer boundary clockwise and summing $IR$ drops (each resistor carries its own mesh current; the $6\,\Omega$ on the boundary carries $I_3-I_4$): $$5I_1+4I_2+3I_3+6\,(I_3-I_4)=0.$$
  3. (a) Mesh-4 KVL. Around mesh $4$ (through the $6\,\Omega$, the $1\,\Omega$ and the $15\text{ V}$ rise): $$6\,(I_4-I_3)+1\cdot I_4+15=0.$$ These four boxed relations are the requested mesh equations.
  4. (b) Reduce and solve. Substituting $I_o=-I_4$ gives $I_3-I_1=-4I_4$. With $I_2=I_1+2$, the super-mesh KVL becomes $5I_1+4(I_1+2)+3I_3+6I_3-6I_4=0\Rightarrow 9I_1+9I_3-6I_4=-8$, and mesh 4 gives $-6I_3+7I_4=-15$. Together with $I_3=I_1-4I_4$ the linear solve yields $$\boxed{I_1=-2.87\text{ A},\ \ I_2=-0.87\text{ A},\ \ I_3=1.29\text{ A},\ \ I_4=-1.04\text{ A}.}$$ Hence $I_o=-I_4=1.04\text{ A}$ (consistent: $I_3-I_1=4.16=4I_o$).
  5. (c) Power in the $6\,\Omega$. Its current is $I_3-I_4=1.29-(-1.04)=2.33\text{ A}$, so $$\boxed{P_{6\Omega}=(I_3-I_4)^2\,(6)=(2.33)^2(6)=32.5\text{ W}.}$$
QuantityValue
$I_1$$-2.87\text{ A}$
$I_2$$-0.87\text{ A}$
$I_3$$1.29\text{ A}$
$I_4$$-1.04\text{ A}$
Control current $I_o$$1.04\text{ A}$
Power in $6\,\Omega$$32.5\text{ W}$