Step 1: Understanding the Concept:
This question describes a series RLC circuit. The current in such a circuit is maximum when the circuit is in a state of resonance. Resonance occurs when the inductive reactance (\(X_L\)) becomes equal to the capacitive reactance (\(X_C\)), causing the total impedance of the circuit to be at its minimum value (equal to the resistance \(R\)).
Step 2: Key Formula or Approach:
The condition for resonance in a series RLC circuit is:
\[ X_L = X_C \]
where \(X_L = 2\pi f L\) is the inductive reactance and \(X_C = \frac{1}{2\pi f C}\) is the capacitive reactance.
By equating these, we get the formula for the resonant frequency, or we can solve for the capacitance \(C\) needed for resonance at a given frequency \(f\).
\[ 2\pi f L = \frac{1}{2\pi f C} \implies C = \frac{1}{(2\pi f)^2 L} = \frac{1}{4\pi^2 f^2 L} \]
Step 3: Detailed Explanation:
Given data:
Inductance, \(L = 500 \, \text{mH} = 500 \times 10^{-3} \, \text{H} = 0.5 \, \text{H}\).
Frequency, \(f = 0.4 \, \text{kHz} = 0.4 \times 10^3 \, \text{Hz} = 400 \, \text{Hz}\).
Calculation:
Substitute the values into the formula for capacitance at resonance:
\[ C = \frac{1}{4\pi^2 f^2 L} \]
\[ C = \frac{1}{4\pi^2 (400)^2 (0.5)} \]
\[ C = \frac{1}{4\pi^2 (160000) (0.5)} \]
\[ C = \frac{1}{2\pi^2 (160000)} = \frac{1}{320000 \pi^2} \, \text{F} \]
Using the approximation \(\pi^2 \approx 9.87\):
\[ C \approx \frac{1}{320000 \times 9.87} = \frac{1}{3158400} \, \text{F} \]
\[ C \approx 3.166 \times 10^{-7} \, \text{F} \]
To express this value in microfarads (µF), we multiply by \(10^6\):
\[ C \approx 3.166 \times 10^{-7} \times 10^6 \, \mu\text{F} = 0.3166 \, \mu\text{F} \]
This value is approximately 0.32 µF.
Step 4: Final Answer:
The required capacitance to achieve maximum current (resonance) is approximately 0.32 µF.