Difficulty: Easy
Correct Answer: Correct
Explanation:
Introduction / Context:
Inductive reactance quantifies how an inductor impedes alternating current due to the changing magnetic field. It plays a central role in AC analysis, filter design, resonance calculations, and impedance matching. The standard relationship ties reactance to frequency and inductance linearly in magnitude.
Given Data / Assumptions:
Concept / Approach:
For a sinusoidal steady state, the inductor voltage-current relation is v(t) = L * di/dt. In phasor form, this becomes V = j ω L * I, where ω = 2π f is the angular frequency. The impedance of the inductor is therefore Z_L = j ω L. The magnitude of this impedance is |Z_L| = ω L = 2π f L, which is by definition the inductive reactance, X_L. Thus, X_L grows linearly with frequency and inductance; at DC (f = 0), X_L = 0 Ω, behaving as a short in ideal form.
Step-by-Step Solution:
Verification / Alternative check:
Example: L = 10 mH at f = 1 kHz → X_L = 2π * 1000 * 0.01 = about 62.8 Ω. A measurement with an LCR meter at 1 kHz would read a similar reactance (ignoring ESR and parasitics).
Why Other Options Are Wrong:
Common Pitfalls:
Forgetting units (henry and hertz) leading to numeric errors; confusing reactance magnitude X_L with the complex impedance j ω L; neglecting nonidealities like winding resistance and self-resonance at very high frequencies.
Final Answer:
Correct
Discussion & Comments