Difficulty: Easy
Correct Answer: Correct
Explanation:
Introduction / Context:Inductors behave differently during transients and in steady-state. In DC steady-state, an ideal inductor has zero voltage across it (di/dt = 0), acting as a short circuit. Therefore, the loop's resistances determine the final current value, a key point in power supply and relay driver design.
Given Data / Assumptions:
Concept / Approach:In steady DC, di/dt = 0 implies v_L = L * 0 = 0. KVL then reduces the loop to the source voltage dropping entirely across resistive elements, so I_DC = V_source / R_total. The inductance value L influenced the transient ramp rate but not the final DC current (for an ideal inductor).
Step-by-Step Solution:
Write v_L = L * di/dt; at steady DC, v_L = 0.Apply KVL: V_source = I * R_total.Solve for I: I = V_source / R_total.Conclude the inductor does not limit DC current; resistance does.Verification / Alternative check:Measure current after a long time in a series RL step response; the final current equals V/R_total, independent of L (though the time constant tau = L/R_total set the rise time).
Why Other Options Are Wrong:
Common Pitfalls:Confusing the time constant (which uses L) with the final steady-state current; overlooking small but present winding resistance in real inductors that should be included in R_total.
Final Answer:Correct
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