In a series RLC circuit comprising a resistor (R), inductor (L), and capacitor (C), resonance occurs when the frequency of the applied voltage aligns with the circuit's natural frequency. This frequency, termed the resonant frequency, allows the current amplitude to reach a maximum, calculated using the equation √(R² + (X_L - X_C)²) where X_L is the inductive reactance and X_C is the capacitive reactance. When resonance is achieved, the total impedance of the circuit minimizes to R, and thus the current amplitude is dictated solely by the source voltage divided by the resistance. The concept of resonance is crucial for many electronic applications, such as tuning circuits in radios, where adjusting capacitance allows the circuit to resonate with desired frequencies.