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Question: The circuit below has an ideal inductor and a switch as shown in figure. The switch can be closed fo...

The circuit below has an ideal inductor and a switch as shown in figure. The switch can be closed for a long time and then can be opened at t = 0 or it can be closed at t = 0. List-I gives the different circuit elements and list-II gives the value.

List-IList-II
(I)Current in inductor(P)6V7\frac{6V}{7}
(II)Voltage across inductor(Q)3V2\frac{3V}{2}
(III)Current supplied by battery(R)V4R\frac{V}{4R}
(IV)Energy stored in the inductor(S)VR\frac{V}{R}
(T)Zero
(U)LV232R2\frac{LV^2}{32R^2}

If the switch was closed at t = 0 then which of the following options are correct match of list I and II for that instant?

A

6V7\frac{6V}{7}

B

3V2\frac{3V}{2}

C

V4R\frac{V}{4R}

D

VR\frac{V}{R}

E

Zero

F

LV232R2\frac{LV^2}{32R^2}

Answer

The correct matches are (I)-T, (II)-P, (IV)-T. The value for (III) is not in List-II.

Explanation

Solution

Here's a breakdown of the solution:

Understanding the Circuit at t = 0+

When the switch is closed at t = 0, we analyze the circuit's behavior immediately after the switch closure (t = 0+). Crucially, the current through an inductor cannot change instantaneously.

Step-by-step Analysis

  1. (I) Current in Inductor:

    • At t = 0+, the inductor acts as an open circuit because the current through it was zero before the switch closed.
    • Therefore, the current in the inductor, IL(0+)=0I_L(0^+) = 0. This matches option (T).
  2. (II) Voltage across Inductor:

    • The voltage across the inductor at t = 0+ can be found by analyzing the equivalent circuit. The inductor branch (L and 3R) is in parallel with the 3R resistor (2R + R). This parallel combination is in series with the R/2 resistor, and the battery V.
    • The current supplied by the battery is I=VR/2+3R=2V7RI = \frac{V}{R/2 + 3R} = \frac{2V}{7R}. This current flows through the 3R resistor.
    • The voltage across the 3R resistor (and therefore across the inductor branch) is V3R=2V7R3R=6V7V_{3R} = \frac{2V}{7R} \cdot 3R = \frac{6V}{7}. Since the inductor current is zero at t=0+, the voltage across the inductor is simply the voltage across the parallel branch, which is 6V7\frac{6V}{7}. This matches option (P).
  3. (III) Current Supplied by Battery:

    • As calculated above, the current supplied by the battery at t = 0+ is 2V7R\frac{2V}{7R}. However, this value is not present in List-II.
  4. (IV) Energy Stored in the Inductor:

    • The energy stored in an inductor is given by E=12LI2E = \frac{1}{2}LI^2.
    • Since the current through the inductor at t = 0+ is zero, the energy stored in the inductor is also zero. This matches option (T).

Conclusion

Based on the analysis, the correct matches are (I)-T, (II)-P, and (IV)-T. The value for (III) is calculated to be 2V7R\frac{2V}{7R}, which is not found in List-II. Therefore, we can only definitively match (I), (II), and (IV).