A 100 $\Omega$ resistor, a 50 $\mu$F capacitor and an inductor are connected in series to an ac source of frequency 50 Hz. If the circuit is in resonance, then the impedance of the circuit is:
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At resonance in an RLC series circuit, impedance equals resistance ($Z = R$), as $X_L = X_C$, canceling out the reactive components.
At resonance in an RLC series circuit, the inductive reactance $X_L$ equals the capacitive reactance $X_C$, so $X_L - X_C = 0$.
The impedance $Z$ of the circuit is then purely resistive: $Z = R$.
Given: $R = 100$ $\Omega$.
Thus, at resonance, $Z = 100$ $\Omega$.