Inductors behave as short circuits after a long time in DC circuits. Use resistor combi nations to calculate the equivalent resistance.
Step 1: Behavior of inductors after a long time After a long time, the inductors behave as short circuits (resistance-less paths) because the current through them becomes steady, and there is no changing magnetic flux.
Step 2: Simplified circuit analysis With the inductors acting as short circuits, the circuit reduces to three resistors connected in parallel across the battery.
Step 3: Equivalent resistance of the parallel resistors The equivalent resistance (\( R_\text{eq} \)) of three identical resistors in parallel is given by:
\[ \frac{1}{R_\text{eq}} = \frac{1}{R} + \frac{1}{R} + \frac{1}{R} \] \[ \frac{1}{R_\text{eq}} = \frac{1}{12} + \frac{1}{12} + \frac{1}{12} = \frac{3}{12} \] \[ R_\text{eq} = \frac{12}{3} = 4 \, \Omega \]
Step 4: Total current through the battery Using Ohm's law, the total current through the battery is:
\[ I = \frac{\text{EMF}}{R_\text{eq}} = \frac{12}{4} = 3 \, \text{A} \]
The correct answer is 3.
After long time an inductor behaves as a resistance-less path.
So current through cell
I=R/312=3A{∵R=12Ω}
Draw the plots showing the variation of magnetic flux φ linked with the loop with time t and variation of induced emf E with time t. Mark the relevant values of E, φ and t on the graphs.
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