Step 1: Understanding the Concept:
For a series LCR circuit, \(Z = \sqrt{R^2 + \left(\omega L - \dfrac1{\omega C}\right)^2}\).
Step 2: Low frequency:
At low frequency \(\dfrac1{\omega C}\) is large, so the reactance is large and capacitive. \(Z\) is large.
Step 3: At resonance:
As \(\omega\) increases, \(\dfrac1{\omega C}\) falls and \(\omega L\) rises until \(\omega L = \dfrac1{\omega C}\), where \(Z = R\), the minimum value.
Step 4: Beyond resonance:
For higher \(\omega\), \(\omega L\) dominates and \(Z\) rises again.
So the impedance first decreases, becomes minimum and then increases, option (D). The other options describe only one part of this behaviour.
Final Answer:
Z dips to R at resonance, then increases again.
\[ \boxed{\text{(D) }\text{first decreases, becomes minimum and then increases}} \]