In a series L-C-R circuit, resonance occurs when the inductive reactance (\( X_L \)) and capacitive reactance (\( X_C \)) are equal in magnitude but opposite in phase. The formula for the resonant frequency \( f_0 \) of a series L-C-R circuit is given by:
\[
f_0 = \frac{1}{2 \pi \sqrt{LC}}
\]
where:
- \( L \) is the inductance in henries (H),
- \( C \) is the capacitance in farads (F).
At this frequency, the impedance of the circuit is purely resistive, and the current reaches its maximum value.