Concept:A \(\pi\)-filter combines capacitive bypassing and inductive choking: the first shunt capacitor (\(C_1\)) bypasses the majority of the AC ripple to ground; the series choke inductor (\(L\)) offers high inductive reactance (\(X_L\)) to block remaining AC ripple; and the second capacitor (\(C_2\)) further smooths residual ripple before the load.
Formula:$$\text{Ripple Factor (}\pi\text{-filter): } r \approx \frac{\sqrt{2}}{8\omega^3 L C_1 C_2 R_L}$$
Solution:- Shunt capacitors \(C_1\) and \(C_2\) have low capacitive reactance (\(X_C = \frac{1}{2\pi f C}\)) to AC ripple, shorting ripple to ground.
- Series choke \(L\) has high inductive reactance (\(X_L = 2\pi f L\)) to AC ripple, blocking ripple from reaching the load.
- For DC (\(f = 0\)), \(X_C = \infty\) (open) and \(X_L = 0\) (short), allowing DC to pass without attenuation.
Why other options are incorrect:- Option A: The primary goal of a power supply filter is to pass DC, not block it.
- Option C: A filter smooths existing rectified waveforms; it does not generate DC electrochemically.
- Option D: Filters attenuate ripple amplitude; they do not alter the fundamental ripple frequency.
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