The circuit shown in the figure with the switch \( S \) open is in steady state. After the switch \( S \) is closed, the time constant of the circuit in seconds is:
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For time constants in \( R-L \) networks:
- Combine resistances using series/parallel rules.
- Combine inductances similarly.
Step 1: Analyzing the circuit after closing the switch.
When the switch \( S \) is closed, the circuit becomes an \( R-L \) network. The time constant (\( \tau \)) of an \( R-L \) circuit is given by:
\[
\tau = \frac{L_{\text{eq}}}{R_{\text{eq}}}.
\]
Step 2: Calculating \( R_{\text{eq}} \) (Thevenin resistance).
The resistances in the circuit are combined as:
\[
R_{\text{eq}} = 1 \, \Omega + 1 \, \Omega = 2 \, \Omega.
\]
Step 3: Calculating \( L_{\text{eq}} \) (equivalent inductance).
The inductors in series are added directly:
\[
L_{\text{eq}} = 1+1+\frac{1}{2} = \frac{5}{2}
\]
Step 4: Determining the time constant (\( \tau \)).
\[
\tau = \frac{L_{\text{eq}}}{R_{\text{eq}}} = \frac{5}{2*2} = \frac{5}{4}=1.25 \, \text{seconds}.
\]
Hence, the correct option is (1) \(1.25 \).