Find i(t) in the circuit of Fig. 7.51 for t > 0 . Assume that the switch has been closed for a long time.
When t < 0 , the 3-Ω resistor is short-circuited, and the inductor acts like a short circuit. The current through the inductor at t = 0^{-} (i.e., just before t = 0 ) is
i(o^{-} ) = \frac{10}{2} = 5 A
Since the inductor current cannot change instantaneously,
i(0) = i(0^{+}) = i(0^{-}) = 5 A
When t > 0 , the switch is open. The 2-Ω and 3-Ω resistors are in series, so that
i(∞) = \frac{10}{2 + 3} = 2 A
The Thevenin resistance across the inductor terminals is
R_{Th} = 2 + 3 = 5 Ω
For the time constant,
\tau = \frac{L}{R_{Th}} = \frac{\frac{1}{3}}{5} = \frac{1}{15} s
Thus,
i(t0 = i ( ∞) + [i(0) – i(∞) ] e^{-t/\tau}
= 2 + (5 – 2) e^{-15t} = 2 + 3 e^{-15t} A , t > o
Check: In Fig. 7.51, for t > 0 , KVL must be satisfied; that is,
10 = 5i + L \frac{di}{dt}
5i + L \frac{di}{dt} = [ 10 + 15 e^{-15t} ] + [ \frac{1}{3} (3) (-15) e^{-15t} ] = 10
This confirms the result.