With phasors proportional to , the resistor, inductor, and capacitor have complex impedances , , and . In a series circuit they carry the same electric current, so their voltage drops add:
The real part describes Joule heating; the imaginary part changes sign between capacitive and inductive response, passing through zero at .
The voltage divider relation for the capacitor output gives the transfer function
Consequently the relative wave amplitude is
For input , the output is , where the continuous phase shift is
For positive frequency and , this phase shift goes from towards , passing through at . A one-argument arctangent without a quadrant correction would wrongly predict a positive phase shift above . The capacitor follows a slowly varying input voltage, while its output falls as at high frequency.
At the inductive and capacitive electrical reactances cancel, so the complex impedance is and the electric current amplitude is . The capacitor voltage amplitude is . Thus the specified quality factor is
A capacitor output exceeding the input voltage is consistent with a passive electrical circuit: the inductor and capacitor voltages largely cancel in their sum. The expression assumes positive ; the ideal undamped limit has no finite steady resonant response.
Put . Maximizing the output wave amplitude is equivalent to minimizing
Its derivative is . An interior minimum at positive frequency therefore requires , and occurs at
Indeed , and the peak value is . For , increases for and the largest output is the DC value . At equality the putative peak has reached zero frequency; there is no distinct nonzero-frequency resonance. This threshold concerns capacitor voltage peaking: the series RLC circuit's electric current still has its maximum at for every positive .

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