Q = √(L/C)/R; f₀ = 1/(2π√(LC))
Quality factor compares resonant reactance with total series resistance.
Quality factor compares resonant reactance with total series resistance.
Select a target and calculate.
Quality factor compares resonant reactance with total series resistance.
R=20 Ω, L=100 mH and C=100 µF give f₀≈50.33 Hz and Q≈1.58.
Linear lumped series RLC circuit with frequency-independent equivalent values; parasitics, loading and tolerances are excluded.
This calculator evaluates how sharply an idealised series circuit selects around resonance. It complements the RLC current calculator with a dimensionless damping and selectivity measure.
At f₀=1/(2π√LC), inductive and capacitive reactance are equal. Series quality Q=ω₀L/R=1/(ω₀CR)=√(L/C)/R compares that reactance with all effective series loss.
Q = √(L/C)/R; f₀ = 1/(2π√(LC))
f₀ = 1/(2π√(LC))Q = ω₀L/RQ = 1/(ω₀CR)Q = √(L/C)/R| Symbol / input | Meaning |
|---|---|
| Quality factor Q | Dimensionless ratio of reactance at resonance to total series resistance. |
| Series resistance R | Total loss-producing series resistance including coil winding, capacitor ESR and wiring. |
| Inductance L | Effective inductance near the calculated resonance frequency. |
| Capacitance C | Effective series capacitance near the calculated resonance frequency. |
R must include every series loss effective at resonance, including winding resistance and capacitor ESR. L and C are effective values near f₀, not unchecked ideal ratings at another frequency.
Estimate L and C, determine f₀, then enter total R effective there. Use Q for option comparison and verify actual response by measurement.
R=20 Ω, L=100 mH and C=100 µF give f₀≈50.33 Hz. √(L/C)=31.62 Ω, so Q≈1.58.
Greater Q means lower relative damping and sharper resonance, but can also create high component voltages and greater tolerance sensitivity.
R in Ω, L with henry prefixes and C with farad prefixes; Q is dimensionless. Resonance follows from coherent SI values.
Teaching resonance and damping, and preliminary comparison of series filters, tuned circuits and laboratory resonators.
Lumped linear equivalent with frequency-independent R, L and C. Source/load damping, parasitics, skin effect, core loss and tolerances are excluded.
Common mistake: Do not use only a drawn resistor while omitting winding and ESR losses. Higher Q is not automatically better because it can create voltage magnification and narrow tolerances.
Teaching resonance and damping, and preliminary comparison of series filters, tuned circuits and laboratory resonators.
R must include every series loss effective at resonance, including winding resistance and capacitor ESR. L and C are effective values near f₀, not unchecked ideal ratings at another frequency.
Lumped linear equivalent with frequency-independent R, L and C. Source/load damping, parasitics, skin effect, core loss and tolerances are excluded.