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Electricity and Electronics · AC Current and Power

Series RLC resonance and impedance

In a series RLC circuit, the reactances of the coil and capacitor cancel each other at a specific frequency. We will examine the conditions under which the current increases with a constant voltage.

Related experiment: Series RLC resonance →
Series RLC resonance
Series RLC resonance: simulation view →

Meaning and mechanism

In AC circuits, inductors and capacitors produce different sizes and phase responses depending on the frequency. The sum of resistance and this effect is impedance.

The reactance of a coil increases as the frequency increases, while the reactance of a capacitor decreases. When their magnitudes are equal, the imaginary part of the sum in a series circuit is canceled out.

Relationships and conditions

Z=R+j(ωL−1/ωC), and the resonant frequency is f₀=1/(2π√LC). In an ideal series circuit with fixed supply voltage and R, current is greatest at resonance.

This result concerns a series circuit in steady state. It does not transfer directly to parallel resonance or real circuits with parasitic elements and frequency-dependent losses.

What to observe in the simulation

At resonance inductive and capacitive reactance cancel and current is maximal.

Only steady state of ideal lumped elements is modeled. Coil losses and parasitic effects are omitted. Experiment on screen; do not reproduce this with real power supplies, outlets or high voltage.

Key relationships and symbols

Z = R + j(ωL−1/(ωC)) · f₀ = 1/(2π√LC)

Symbols and units used in the formulas
SymbolMeaningUnit
ZComplex impedanceΩ
ωAngular frequency 2πfrad/s
L, CInductance and capacitanceH, F

Worked example

At resonance, what is the RMS current for a 6 V RMS input and 20 Ω resistance?

0.3 A

Common misconceptions

  • In a resonance circuit, neither the inductor nor the capacitor will have a voltage of 0.

Explore this concept through experiments

References

OpenStax · University Physics Volume 2 (English)