Consider the RL circuit shown in Figure A2. i1 and i2 are the currents in each loop, which satisfy the
differential equations
L1dtdi1+R2(i1−i2)+R1i1=v(t)(A3a)
L2dtdi2+R2(i2−i1)=0(A3b)
Assume L1=0.8 H, L2=1 H, R1=1.4 Ω, R2=1 Ω and v(t)=100 V for t>0. The
initial conditions are i1(0)=0 and i2(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.Formulas you may need
- L[dtdi]=sI(s)−i(0); constant 100→s100 (learn this; printed in the ENGR201 Laplace table)
- eat↔s−a1 (learn this; printed in the ENGR201 Laplace table)
- Cover-up rule for distinct poles: residue at s=p is [(s−p)F(s)]s=p (learn this)
- Final value theorem limt→∞i(t)=lims→0sI(s) (learn this)
- (a)
Find the Laplace transforms of the currents.
[10]2:1 - (b)
Find the currents by the inverse Laplace transform.
[12] - (c)
Explain what happens to the currents when
t increases.
[3]2:2