ENGR201 2023 A2Past paperOld spec ENGR201First25 marks30 min

ENGR201 Engineering Analysis 2023 Section A, A2[VALID] official answers

Consider the RL circuit shown in Figure A2. i1i_1 and i2i_2 are the currents in each loop, which satisfy the differential equations

L1di1dt+R2(i1−i2)+R1i1=v(t)(A3a)L_1\frac{di_1}{dt} + R_2(i_1 - i_2) + R_1 i_1 = v(t) \qquad \text{(A3a)} L2di2dt+R2(i2−i1)=0(A3b)L_2\frac{di_2}{dt} + R_2(i_2 - i_1) = 0 \qquad \text{(A3b)}

Assume L1=0.8L_1 = 0.8 H, L2=1L_2 = 1 H, R1=1.4 ΩR_1 = 1.4\ \Omega, R2=1 ΩR_2 = 1\ \Omega and v(t)=100v(t) = 100 V for t>0t > 0. The initial conditions are i1(0)=0i_1(0) = 0 and i2(0)=0i_2(0) = 0.

Figure A2: two-loop circuit; loop 1 (current i1) contains v(t), R1, L1 and the shared R2; loop 2 (current i2) contains R2 and L2.
Figure A2: two-loop circuit; loop 1 (current i1) contains v(t), R1, L1 and the shared R2; loop 2 (current i2) contains R2 and L2.
Formulas you may need
  • L[didt]=sI(s)−i(0)\mathcal{L}\left[\dfrac{di}{dt}\right] = sI(s) - i(0); constant 100→100s100 \to \dfrac{100}{s} (learn this; printed in the ENGR201 Laplace table)
  • eat↔1s−ae^{at} \leftrightarrow \dfrac{1}{s - a} (learn this; printed in the ENGR201 Laplace table)
  • Cover-up rule for distinct poles: residue at s=ps = p is [(s−p)F(s)]s=p\left[(s - p)F(s)\right]_{s = p} (learn this)
  • Final value theorem lim⁡t→∞i(t)=lim⁡s→0sI(s)\lim_{t \to \infty} i(t) = \lim_{s \to 0} sI(s) (learn this)
  1. (a)
    Find the Laplace transforms of the currents.
    [10]2:1
  2. (b)
    Find the currents by the inverse Laplace transform.
    [12]
  3. (c)
    Explain what happens to the currents when tt increases.
    [3]2:2