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04-BS-4 · May 2016

Question 1 of 7: DC Bridge Network — KCL/KVL and an Unknown Source Current

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

Notes on this paper

National Exams, 04-BS-4 Electric Circuits and Power — May 2016. Closed book; one double-sided aid sheet permitted; any five of the seven questions constitute a complete paper (all seven are answered here as a complete study resource).

Reference texts: Sadiku & Alexander, Fundamentals of Electric Circuits, 6th ed. (circuit analysis, transients, AC steady state, magnetic circuits); Boylestad & Nashelsky, Electronic Devices and Circuit Theory (rectifiers); Mano, Digital Design (combinational logic).

Question 1: DC Bridge Network — KCL/KVL and an Unknown Source Current (20 marks)

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. The bridge-style DC network of Figure 1 has an ideal voltage source V6 across node A and the ground rail, an unknown ideal current source I5 between node B and ground, and four resistors as tabulated. A measurement shows I4 = 2 A in the branch through R4.

Given data
QuantityValue
R110 Ω
R211 Ω
R32 Ω
R45 Ω
V650 V
I4 (measured)2 A

Find. The KCL/KVL equations at the labelled nodes and loops, the unknown source current I5, and the power dissipated in R1.

I1I4CR1R3I3R2I2AB+−V6I5R4I6D
Figure 1: DC bridge circuit (R1=10, R2=11, R3=2, R4=5, V6=50V, I4=2 A)

Approach. Node C connects to the ground rail only through R4, so the measured I4 fixes VC directly; V6 fixes VA directly since it is an ideal source; walking those two fixed potentials through R1 and R3 isolates I5 from a single KCL equation at node B.

  1. KCL at nodes A, B, C (part a). Taking currents leaving each node as positive: $$ \text{Node A: } I_1 + I_2 = I_6 \qquad \text{Node B: } I_2 + I_5 = I_3 \qquad \text{Node C: } I_1+I_3 = I_4 $$ (I1 through R1, I2 through R2, I3 through R3, I4 through R4, I5 the unknown source, I6 through V6.)
  2. KVL for the three loops (part b). Walking each loop and summing voltage drops to zero: $$ \text{Loop ACBA: } I_1R_1 - I_3R_3 - I_2R_2 = 0 $$ $$ \text{Loop ACDA: } I_1R_1 + I_4R_4 - V_6 = 0 $$ $$ \text{Loop ABCDA: } I_2R_2 + I_3R_3 + I_4R_4 - V_6 = 0 $$ (the third loop is the sum of the first two and is not independent, but the exam asks for all three.)
  3. Fix the two known nodes. The ideal source gives $V_A = V_6 = 50\text{ V}$ directly. Node C reaches ground only through R4, so the measurement fixes $$ V_C = I_4R_4 = (2\text{ A})(5\ \Omega) = 10\text{ V}. $$ Then $ I_1 = \dfrac{V_A-V_C}{R_1} = \dfrac{50-10}{10} = \boxed{4\text{ A}}. $
  4. KCL at C, then Ohm's law on R3. From node C, $I_3 = I_4-I_1 = 2-4 = -2\text{ A}$ (the physical current in R3 runs from C down to B, opposite the assumed reference). Since $I_3=(V_B-V_C)/R_3$, $$ V_B = V_C + I_3R_3 = 10 + (-2)(2) = 6\text{ V}. $$
  5. Ohm's law on R2, then KCL at B for I5 (part c). $$ I_2 = \frac{V_A-V_B}{R_2} = \frac{50-6}{11} = 4\text{ A}. $$ From the node-B equation, $ I_5 = I_3 - I_2 = -2-4 = \boxed{-6\text{ A}}$ — magnitude 6 A, directed opposite to the assumed "into B" reference arrow (i.e. the source actually delivers 6 A from node B down to the ground rail).
  6. Power in R1 (part d). $$ P_{R_1} = I_1^2R_1 = (4)^2(10) = \boxed{160\text{ W}}. $$
Final results
QuantityValue
VA50 V
VC10 V
VB6 V
I14 A
I24 A
I3−2 A
I4 (given)2 A
I5−6 A
PR1160 W
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