Difficulty: Easy
Correct Answer: The circuit is at resonance
Explanation:
Introduction:
Resonance in RLC circuits is a cornerstone concept: it occurs when the inductive and capacitive reactances cancel each other in magnitude (X_L = X_C). Recognizing this condition helps predict current, voltage distribution, and power factor behavior in both series and parallel topologies.
Given Data / Assumptions:
Concept / Approach:
At resonance, the net reactive component of impedance is zero in series circuits (Z is purely resistive), or the net reactive component of admittance is zero in parallel circuits (Y is purely conductive). This is the unifying definition of resonance and is directly tied to X_L = X_C.
Step-by-Step Solution:
Write X_L = ωL and X_C = 1 / (ωC)Set X_L = X_C ⇒ ωL = 1 / (ωC)Solve for resonance radian frequency: ω_0 = 1 / sqrt(L * C)Thus f_0 = ω_0 / (2 * π) = 1 / (2 * π * sqrt(L * C))At f_0, the reactive effects cancel, defining resonance.
Verification / Alternative check:
Series RLC: Z = R + j(X_L − X_C) ⇒ at resonance Z = R (minimum magnitude), current is maximized for a given applied voltage. Parallel RLC: input admittance Y has zero imaginary part at resonance, leading to minimum source current. In both cases, the defining condition is X_L = X_C.
Why Other Options Are Wrong:
Common Pitfalls:
Final Answer:
The circuit is at resonance
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