Electrical Circuits · Transients and AC

Series RLC resonance

Understand resonance in a series RLC circuit: resonant frequency, quality factor, bandwidth and phase.

By the end of this topic you will be able to

  • Calculate inductive and capacitive reactance and the impedance of a series RLC circuit.
  • Find the resonant frequency, quality factor and bandwidth.
  • Explain why the current peaks at resonance and what the phase angle shows.

Reactance

In an AC circuit, inductors and capacitors oppose current by an amount that depends on frequency. This opposition is called reactance.

XL=2πfL,XC=12πfCX_L = 2\pi f L, \qquad X_C = \frac{1}{2\pi f C}

An inductor's reactance grows with frequency (it resists rapid changes in current); a capacitor's falls with frequency (it passes rapid changes more easily). Both are in ohms.

Series RLC impedance

The total opposition of a resistor, inductor and capacitor in series is the impedance:

|Z|=R2+(XL−XC)2|Z| = \sqrt{R^2 + (X_L - X_C)^2}

XLX_L and XCX_C work against each other: the inductor's voltage and the capacitor's voltage are in opposite phase, so they partly cancel.

Resonance

At the particular frequency where XL=XCX_L = X_C, the two reactances cancel completely and the impedance is just RR, its minimum value. The current is then at its maximum, V/RV/R, and is in phase with the supply voltage. This is resonance:

f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}

Quality factor and bandwidth

The quality factor QQ measures how sharp the resonance peak is:

Q=1RLC,bandwidth=f0QQ = \frac{1}{R}\sqrt{\frac{L}{C}}, \qquad \text{bandwidth} = \frac{f_0}{Q}

A small resistance gives a high QQ, a tall narrow peak, which is good for a radio tuner that must pick one station among many. The bandwidth is the width of the band over which the current is at least 1/21/\sqrt2 (0.707) of its peak value (the half-power points).

Phase

Below f0f_0 the circuit is capacitive (current leads voltage, φ<0\varphi < 0); above f0f_0 it is inductive (current lags, φ>0\varphi > 0). At resonance φ=0\varphi = 0.

Interactive modelSlide the frequency across resonance, then change R to see the peak widen or sharpen.

This interactive model needs JavaScript. The theory, worked example and problems on this page work without it.

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Practice problems

  1. Find the resonant frequency for L=1L = 1 mH and C=1μFC = 1\ \mu\text{F}.
    Show answer
    f0=1/(2π10−9)=5033f_0 = 1/(2\pi\sqrt{10^{-9}}) = 5033 Hz.
  2. A circuit has R=5ΩR = 5\ \Omega, L=10L = 10 mH and C=10μFC = 10\ \mu\text{F}. Find QQ.
    Show answer
    Q=(1/5)0.01/(10×10−6)=31.6/5=6.3Q = (1/5)\sqrt{0.01/(10\times10^{-6})} = 31.6/5 = 6.3.
  3. In the model, if you double R, what happens to the peak current and to the bandwidth?
    Show answer
    The peak current halves (V/RV/R), and the bandwidth doubles (BW =f0/Q= f_0/Q and Q∝1/RQ \propto 1/R).
  4. At 0.5 f0f_0 is the circuit inductive or capacitive?
    Show answer
    Capacitive, as XC>XLX_C > X_L below resonance (the current leads the voltage).

Key formulae

Inductive reactance
XL=2πfLX_L = 2\pi f L
Capacitive reactance
XC=12πfCX_C = \frac{1}{2\pi f C}
Impedance
|Z|=R2+(XL−XC)2|Z| = \sqrt{R^2 + (X_L - X_C)^2}
Resonant frequency
f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}
Quality factor and bandwidth
Q=1RLC,BW=f0QQ = \frac{1}{R}\sqrt{\frac{L}{C}}, \quad \text{BW} = \frac{f_0}{Q}
Phase angle
φ=tan−1XL−XCR\varphi = \tan^{-1}\frac{X_L - X_C}{R}
Lecturer notes: suggested plan, activity and assessment

Suggested plan (45 min). 5 min: tuning a radio; 15 min: reactance, impedance, cancelling; 10 min: resonance and Q; 15 min: model (frequency sweep, resistance sweep).

Activity. Challenge: choose L and C to resonate at 1 kHz with a Q of 5; check in the model.

Discussion. Where are resonant circuits used? (Tuners, filters, wireless charging, induction heating.)

Assessment idea. Calculate bandwidth and half-power frequencies for given R, L, C.