Level 4 — ApplicationCircuit Analysis Fundamentals

Circuit Analysis Fundamentals

60 minutes60 marksprintable — key stays hidden on paper

Level 4 — Application (novel problems, no hints) Time limit: 60 minutes Total marks: 60

Answer all questions. Show all working. Use ...... notation for intermediate results where helpful.


Question 1 — Mixed Network + Divider (12 marks)

A 24 V24\text{ V} ideal source drives the following network. From the source, resistor R1=100 ΩR_1 = 100\ \Omega is in series with a parallel combination of R2=300 ΩR_2 = 300\ \Omega and a branch consisting of R3=200 ΩR_3 = 200\ \Omega in series with R4=400 ΩR_4 = 400\ \Omega.

(a) Compute the total equivalent resistance seen by the source. (4) (b) Compute the total current delivered by the source. (2) (c) Compute the current flowing through R4R_4. (3) (d) Compute the voltage across R2R_2. (3)


Question 2 — Thevenin + Load (14 marks)

Consider a two-terminal network across output terminals A–B. A 12 V12\text{ V} source connects through Ra=2 kΩR_a = 2\ \text{k}\Omega to node A; from node A a resistor Rb=6 kΩR_b = 6\ \text{k}\Omega goes to ground (terminal B). A second resistor Rc=3 kΩR_c = 3\ \text{k}\Omega connects node A to terminal A' where a 6 V6\text{ V} source (referenced to ground) is applied.

Treat terminals A and B as the output port (A being node A itself, B being ground).

(a) Find the Thevenin voltage VthV_{th} at A–B (open circuit) using superposition. (6) (b) Find the Thevenin resistance RthR_{th}. (3) (c) A load RL=4 kΩR_L = 4\ \text{k}\Omega is connected across A–B. Find the load current and the power delivered to RLR_L. (3) (d) State the Norton equivalent (INI_N, RNR_N). (2)


Question 3 — RC Transient (12 marks)

A capacitor C=4.7 μFC = 4.7\ \mu\text{F}, initially uncharged, is connected at t=0t=0 through R=10 kΩR = 10\ \text{k}\Omega to a 5 V5\text{ V} supply.

(a) Give the time constant τ\tau. (2) (b) Write the expression for vC(t)v_C(t) and compute vCv_C at t=30 mst = 30\ \text{ms}. (4) (c) Find the time at which the capacitor voltage first reaches 4 V4\text{ V}. (3) (d) At t=0+t = 0^+, what is the current through RR? At tt \to \infty? (3)


Question 4 — RL Transient (10 marks)

An inductor L=50 mHL = 50\ \text{mH} in series with R=25 ΩR = 25\ \Omega is switched onto a 10 V10\text{ V} DC source at t=0t=0 (zero initial current).

(a) Find the time constant and the final steady-state current. (3) (b) Write i(t)i(t) and evaluate it at t=2 mst = 2\ \text{ms}. (4) (c) Find the voltage across the inductor at t=2 mst = 2\ \text{ms}. (3)


Question 5 — AC Reactance (12 marks)

A series RC circuit with R=1 kΩR = 1\ \text{k}\Omega and C=100 nFC = 100\ \text{nF} is driven by a sinusoidal source of RMS voltage 5 V5\text{ V} at frequency f=1592 Hzf = 1592\ \text{Hz} (take ω=2πf104 rad/s\omega = 2\pi f \approx 10^4\ \text{rad/s}).

(a) Compute the capacitive reactance XCX_C. (3) (b) Compute the magnitude of the total impedance Z|Z|. (3) (c) Compute the RMS current magnitude. (3) (d) Compute the phase angle of the current relative to the source voltage. (3)

Answer keyMark scheme & solutions

Question 1

(a) Branch R3+R4=200+400=600 ΩR_3+R_4 = 200+400 = 600\ \Omega. Parallel with R2=300R_2=300: Rp=300600300+600=180000900=200 Ω.R_p = \frac{300\cdot600}{300+600} = \frac{180000}{900} = 200\ \Omega. Total Req=R1+Rp=100+200=300 ΩR_{eq} = R_1 + R_p = 100 + 200 = 300\ \Omega. (4) Why: series adds; parallel uses product/sum; the divider branch is a single series resistance before paralleling.

(b) Itot=24/300=0.08 A=80 mAI_{tot} = 24/300 = 0.08\ \text{A} = 80\ \text{mA}. (2)

(c) Voltage across the parallel block =ItotRp=0.08200=16 V= I_{tot}\cdot R_p = 0.08\cdot200 = 16\ \text{V}. Current through the 600 Ω600\ \Omega branch (through R4R_4): 16/600=0.02667 A=26.7 mA16/600 = 0.02667\ \text{A} = 26.7\ \text{mA}. (3) Why: same voltage across both parallel branches; branch current = branch voltage / branch resistance.

(d) Voltage across R2R_2 equals the parallel-block voltage =16 V= 16\ \text{V}. (3) Why: R2R_2 is directly across the parallel node pair.


Question 2

(a) Superposition at node A (open circuit, no load current drawn since RcR_c path carries current to the 6 V source).

With A open, current can still flow through the path 12VRaARc6V12\text{V}\to R_a\to A\to R_c\to 6\text{V} and through RbR_b to ground. Node equation at A (open output): VA122+VA06+VA63=0(kΩ).\frac{V_A-12}{2} + \frac{V_A-0}{6} + \frac{V_A-6}{3} = 0 \quad (\text{k}\Omega). Multiply by 6: 3(VA12)+VA+2(VA6)=03(V_A-12) + V_A + 2(V_A-6) = 0 3VA36+VA+2VA12=06VA=48VA=8 V.3V_A - 36 + V_A + 2V_A - 12 = 0 \Rightarrow 6V_A = 48 \Rightarrow V_A = 8\ \text{V}. So Vth=8 VV_{th} = 8\ \text{V}. (6) Why: KCL/nodal analysis (equivalent to superposition of the two sources) gives the open-circuit terminal voltage.

(b) Deactivate sources (short both voltage sources). Then from node A three resistors go to ground: RaR_a, RbR_b, RcR_c all in parallel: Rth=(12+16+13)1kΩ=(3+1+26)1=1 kΩ.R_{th} = \left(\tfrac1{2}+\tfrac1{6}+\tfrac1{3}\right)^{-1}\text{k}\Omega = \left(\tfrac{3+1+2}{6}\right)^{-1} = 1\ \text{k}\Omega. (3)

(c) With RL=4 kΩR_L = 4\ \text{k}\Omega: IL=VthRth+RL=81+4=1.6 mA.I_L = \frac{V_{th}}{R_{th}+R_L} = \frac{8}{1+4} = 1.6\ \text{mA}. PL=IL2RL=(1.6×103)24000=0.01024 W10.24 mW.P_L = I_L^2 R_L = (1.6\times10^{-3})^2 \cdot 4000 = 0.01024\ \text{W} \approx 10.24\ \text{mW}. (3)

(d) RN=Rth=1 kΩR_N = R_{th} = 1\ \text{k}\Omega; IN=Vth/Rth=8/1=8 mAI_N = V_{th}/R_{th} = 8/1 = 8\ \text{mA}. (2)


Question 3

(a) τ=RC=1044.7×106=0.047 s=47 ms\tau = RC = 10^4 \cdot 4.7\times10^{-6} = 0.047\ \text{s} = 47\ \text{ms}. (2)

(b) vC(t)=5(1et/τ)v_C(t) = 5\left(1 - e^{-t/\tau}\right). At t=30 mst = 30\ \text{ms}: t/τ=0.030/0.047=0.6383t/\tau = 0.030/0.047 = 0.6383, e0.6383=0.5282e^{-0.6383} = 0.5282. vC=5(10.5282)=2.359 Vv_C = 5(1-0.5282) = 2.359\ \text{V}. (4)

(c) 4=5(1et/τ)et/τ=0.2t=τln5=0.0471.6094=0.0756 s75.6 ms4 = 5(1-e^{-t/\tau}) \Rightarrow e^{-t/\tau} = 0.2 \Rightarrow t = \tau\ln 5 = 0.047\cdot1.6094 = 0.0756\ \text{s} \approx 75.6\ \text{ms}. (3)

(d) At t=0+t=0^+: capacitor acts as short, i=5/10k=0.5 mAi = 5/10\text{k} = 0.5\ \text{mA}. At tt\to\infty: capacitor fully charged, i=0i = 0. (3)


Question 4

(a) τ=L/R=0.05/25=0.002 s=2 ms\tau = L/R = 0.05/25 = 0.002\ \text{s} = 2\ \text{ms}. Final current I=10/25=0.4 AI_\infty = 10/25 = 0.4\ \text{A}. (3)

(b) i(t)=0.4(1et/τ)i(t) = 0.4(1-e^{-t/\tau}). At t=2 ms=τt = 2\ \text{ms} = \tau: i=0.4(1e1)=0.4(0.6321)=0.2528 Ai = 0.4(1-e^{-1}) = 0.4(0.6321) = 0.2528\ \text{A}. (4)

(c) vL=Ldi/dt=Vsourceet/τ=10e1=3.679 Vv_L = L\,di/dt = V_{source}\,e^{-t/\tau} = 10\,e^{-1} = 3.679\ \text{V}. (Check: vR=iR=0.252825=6.32 Vv_R = i R = 0.2528\cdot25 = 6.32\ \text{V}; vL+vR=10 Vv_L + v_R = 10\ \text{V} ✓.) (3)


Question 5

(a) XC=1ωC=1104100×109=1103=1000 ΩX_C = \dfrac{1}{\omega C} = \dfrac{1}{10^4 \cdot 100\times10^{-9}} = \dfrac{1}{10^{-3}} = 1000\ \Omega. (3)

(b) Z=R2+XC2=10002+10002=10002=1414.2 Ω|Z| = \sqrt{R^2 + X_C^2} = \sqrt{1000^2 + 1000^2} = 1000\sqrt2 = 1414.2\ \Omega. (3)

(c) Irms=V/Z=5/1414.2=3.536 mAI_{rms} = V/|Z| = 5/1414.2 = 3.536\ \text{mA}. (3)

(d) For series RC, current leads voltage by θ=arctan(XC/R)=arctan(1)=45\theta = \arctan(X_C/R) = \arctan(1) = 45^\circ (current leads). (3)


[
  {"claim":"Q1 Req = 300 ohm and R4 current = 24/300 * 200 / 600 A","code":"Rp=(300*600)/(300+600); Req=100+Rp; Itot=24/Req; Vpar=Itot*Rp; I_R4=Vpar/600; result = (Req==300) and abs(I_R4-0.026666666666)<1e-6"},
  {"claim":"Q2 Vth=8V, Rth=1k, load current 1.6mA","code":"VA=Rational(48,6); Rth=1/(Rational(1,2)+Rational(1,6)+Rational(1,3)); IL=8/(Rth+4); result = (VA==8) and (Rth==1) and (IL==Rational(8,5)/1000*1000/1000 or abs(float(IL)-1.6)<1e-9)"},
  {"claim":"Q3 vC at 30ms and t for 4V","code":"tau=10**4*4.7e-6; vc=5*(1-exp(-0.030/tau)); t4=tau*ln(5); result = abs(float(vc)-2.3592)<1e-3 and abs(float(t4)-0.07564)<1e-4"},
  {"claim":"Q5 |Z|, I, phase","code":"Xc=1/(10**4*100e-9); Z=sqrt(1000**2+Xc**2); I=5/Z; th=atan(Xc/1000); result = abs(float(Xc)-1000)<1e-6 and abs(float(Z)-1414.2135)<1e-2 and abs(float(I)-0.0035355)<1e-6 and abs(float(th)-pi/4)<1e-9"}
]