In a series LCR circuit, resonance is achieved when inductive reactance ($X_L$) equals capacitive reactance ($X_C$), meaning $X_L = X_C$. This condition leads to:
\[
\omega L = \frac{1}{\omega C} \Rightarrow \omega^2 = \frac{1}{LC} \Rightarrow \omega = \frac{1}{\sqrt{LC}}
\]
At this resonant frequency:
- The net reactance, $X = X_L - X_C$, becomes 0. Consequently, the impedance, $Z$, equals the resistance, $R$ ($Z=R$).
- Therefore, the circuit exhibits behavior characteristic of a pure resistive circuit during resonance.
Based on these findings:
- The assertion is valid.
- The reason provided is also valid.
- The reason accurately elucidates the assertion.
Final answer: Option (A)