In a series RLC circuit, at resonance the impedance is purely resistive and approximately equal to the resistor value.

At resonance, the impedance is maximum.

At resonance, the impedance is zero.

At resonance, the impedance is purely resistive and approximately equal to R.

In a series RLC circuit, resonance happens when the inductor’s reactance and the capacitor’s reactance cancel each other out, so the total impedance becomes purely real and equal to the resistance, Z = R. Because the reactive part drops to zero, the current for a given applied voltage is I = V/R, which is as large as the circuit allows for that R value. In an ideal case this impedance is exactly R; in real circuits small parasitics make it very close to R, hence “approximately equal to the resistor value.” The other statements don’t fit: the impedance is not maximum at resonance (the reactive cancellation makes it minimum, equal to R), it is not zero unless R is zero, and the current is not minimized—it's maximized for the given voltage.

At resonance, the current is minimized.

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