Step 1: Understanding the Concept:
In a series LCR circuit, current and voltage are in phase when the inductive reactance equals the capacitive reactance (resonance).
Step 2: Key Formula or Approach:
\[ \omega^2 LC = 1 \Rightarrow C = \frac{1}{\omega^2L} \]
Step 3: Calculate.
\(\omega = 2\pi f = 2\pi\times 50 = 100\pi\) rad/s, and \(L = \dfrac{4}{\pi^2}\) H.
\[ \omega^2L = 10^4\pi^2\times\frac{4}{\pi^2} = 4\times 10^4 \]
\[ C = \frac{1}{4\times 10^4} = 2.5\times 10^{-5}\text{ F} = 25\ \mu\text{F} \]
Step 4: Check the options.
Only 25 \(\mu\)F matches. The resistance and the supply voltage do not matter at resonance.
Final Answer:
The capacitance is 25 \(\mu\)F, option (D).
\[ \boxed{25\ \mu\text{F}} \]