Resonance in a Series LCR Circuit
Resonance in a series LCR circuit occurs when inductive reactance equals capacitive reactance, making impedance minimum and current maximum.
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Student-friendly explanation
At resonance, XL = XC. Therefore the net reactance XL - XC becomes zero and the circuit behaves like a pure resistor. The impedance becomes Z = R, which is its minimum value, so current reaches its maximum value Imax = Vrms/R. The resonant angular frequency is omega0 = 1/sqrt(LC). A sharp resonance means current changes greatly for a small change in frequency, and this sharpness is measured using the quality factor Q.
How to write this in exams
- 1
Start with the exact idea
Resonance in a series LCR circuit occurs when inductive reactance equals capacitive reactance, making impedance minimum and current maximum.
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Then show how to use it
Set XL = XC. Substitute omega L = 1/(omega C). Solve for omega0. Convert to f0 if required. At resonance, take Z = R and calculate current using RMS voltage. Add the physical meaning: current maximum and circuit purely resistive.
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Add one concrete example
Radio tuning uses resonance. A receiver selects a particular frequency when its LC circuit resonates with the frequency of the desired signal.
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Avoid this incomplete answer
Using omega0 = sqrt(LC) is wrong because the correct relation is the reciprocal square root, omega0 = 1/sqrt(LC).
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Why is current maximum at resonance in a series LCR circuit?
Current is maximum at resonance because XL equals XC, so the net reactance becomes zero. The impedance reduces to R, its minimum value, and therefore I = Vrms/R becomes maximum.
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