Often called the quality factor of a circuit, Q is defined in various ways, depending upon the particular application. In the simple RL and RC series circuits, Q is the ratio of reactance to resistance, as in Eqs. (1),
1. 
where XL is the inductive reactance, XC is the capacitive reactance, and R is the resistance. An important application lies in the dissipation factor or loss angle when the constants of a coil or capacitor are measured by means of the alternating-current bridge.
Q has greater practical significance with respect to the resonant circuit, and a basic definition is given by Eq. (2),
2. 
where Q0 means evaluation at resonance. For certain circuits, such as cavity resonators, this is the only meaning Q can have.
For the RLC series resonant circuit with resonant frequency f0, Eq. (3)
3. 
holds, where R is the total circuit resistance, L is the inductance, and C is the capacitance. Q0 is the Q of the coil if it contains practically the total resistance R. The greater the value of Q0, the sharper will be the resonance peak.
The practical case of a coil of high Q0 in parallel with a capacitor also leads to Q0 = 2πf0L/R. R is the total series resistance of the loop, although the capacitor branch usually has negligible resistance.
In terms of the resonance curve, Eq. (4) holds,
4. 
where f0 is the frequency at resonance, and f1 and f2 are the frequencies at the half-power points. See also Resonance (alternating-current circuits).