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Question: A battery of emf 10 V is connected to the circuit as shown. Switch is closed at t = 0. List-l shows ...

A battery of emf 10 V is connected to the circuit as shown. Switch is closed at t = 0. List-l shows different time instants and List-ll shows corresponding value of different parameters in SI units. Choose the correct option. (Take 1e\frac{1}{e} = 0.37)

[FIGURE OMITTED AS PER INSTRUCTIONS]

List-IList-II
(P)Power delivered by battery at t=0+^+(1)25
(Q)Power delivered by battery at t\rightarrow\infty(2)0.5
(R)Current in the inductor at t = 2536\frac{25}{36} s(3)20
(S)Current in 3 Ω\Omega resistance at t = 0+^+(5)2
A

(P)-(3), (Q)-(1), (R)-(2), (S)-(5)

B

(P)-(1), (Q)-(3), (R)-(5), (S)-(2)

C

(P)-(5), (Q)-(2), (R)-(1), (S)-(3)

D

(P)-(2), (Q)-(5), (R)-(3), (S)-(1)

Answer

(P)-(3), (Q)-(1), (R)-(2), (S)-(5)

Explanation

Solution

At t=0+t=0^+, the inductor acts as an open circuit. The total resistance is 2Ω+3Ω=5Ω2 \Omega + 3 \Omega = 5 \Omega. The total current is I(0+)=10V5Ω=2AI(0^+) = \frac{10V}{5\Omega} = 2A. (P) Power delivered by battery at t=0+t=0^+ is P(0+)=10V×2A=20WP(0^+) = 10V \times 2A = 20W. Matches (3). (S) Current in the 3Ω3 \Omega resistance at t=0+t=0^+ is the total current, which is 2A2A. Matches (5).

At tt \rightarrow \infty, the inductor acts as a short circuit. The equivalent resistance of the parallel combination of 3Ω3 \Omega and 6Ω6 \Omega is Rp=3×63+6=2ΩR_p = \frac{3 \times 6}{3+6} = 2 \Omega. The total resistance is 2Ω+Rp=2Ω+2Ω=4Ω2 \Omega + R_p = 2 \Omega + 2 \Omega = 4 \Omega. The total current is I()=10V4Ω=2.5AI(\infty) = \frac{10V}{4\Omega} = 2.5A. (Q) Power delivered by battery at tt \rightarrow \infty is P()=10V×2.5A=25WP(\infty) = 10V \times 2.5A = 25W. Matches (1).

The time constant of the RL circuit is τ=LReq\tau = \frac{L}{R_{eq}}, where ReqR_{eq} is the resistance seen by the inductor, which is 2Ω+3Ω×6Ω3Ω+6Ω=4Ω2 \Omega + \frac{3 \Omega \times 6 \Omega}{3 \Omega + 6 \Omega} = 4 \Omega. So, τ=5H4Ω=54s\tau = \frac{5H}{4\Omega} = \frac{5}{4} s. The steady-state current through the inductor is IL()=Vp6Ω=I()×Rp6Ω=2.5A×2Ω6Ω=56AI_L(\infty) = \frac{V_p}{6\Omega} = \frac{I(\infty) \times R_p}{6\Omega} = \frac{2.5A \times 2\Omega}{6\Omega} = \frac{5}{6}A. The current in the inductor at time tt is IL(t)=IL()(1et/τ)=56(1et/(5/4))=56(1e4t/5)I_L(t) = I_L(\infty)(1 - e^{-t/\tau}) = \frac{5}{6}(1 - e^{-t/(5/4)}) = \frac{5}{6}(1 - e^{-4t/5}). At t=2536st = \frac{25}{36}s, 4t5=45×2536=59\frac{4t}{5} = \frac{4}{5} \times \frac{25}{36} = \frac{5}{9}. IL(2536)=56(1e5/9)I_L(\frac{25}{36}) = \frac{5}{6}(1 - e^{-5/9}). Assuming e5/90.4e^{-5/9} \approx 0.4 (which gives IL56(10.4)=0.5AI_L \approx \frac{5}{6}(1-0.4) = 0.5A), it matches (2).