Step 1: Understanding the Concept:
Peak Inverse Voltage (PIV) is the maximum reverse voltage that a diode in a rectifier circuit must be able to withstand without breaking down. For a simple half-wave rectifier, during the negative half-cycle of the input AC voltage, the diode is reverse-biased. The maximum voltage it experiences is the peak voltage of the AC waveform at the secondary of the transformer.
Step 2: Key Formula or Approach:
1. Calculate the RMS voltage at the secondary of the transformer (\(V_{s,rms}\)).
2. Calculate the peak voltage at the secondary (\(V_{s,peak}\)).
3. For a half-wave rectifier, PIV = \(V_{s,peak}\).
The relevant formulas are:
\[ \frac{V_s}{V_p} = \frac{N_s}{N_p} \implies V_{s,rms} = V_{p,rms} \times \frac{N_s}{N_p} \]
\[ V_{peak} = V_{rms} \times \sqrt{2} \]
Step 3: Detailed Explanation:
1. Find the secondary RMS voltage (\(V_{s,rms}\)):
The primary voltage is given as \(V_{p,rms} = 220\) V.
The turns ratio is given as 20:1, which means \( \frac{N_p}{N_s} = \frac{20}{1} \).
\[ V_{s,rms} = V_{p,rms} \times \frac{N_s}{N_p} = 220 \, V \times \frac{1}{20} = 11 \, V \]
2. Find the secondary peak voltage (\(V_{s,peak}\)):
The relationship between peak voltage and RMS voltage for a sinusoidal AC supply is:
\[ V_{s,peak} = V_{s,rms} \times \sqrt{2} \]
\[ V_{s,peak} = 11 \, V \times \sqrt{2} \approx 11 \times 1.414 \]
\[ V_{s,peak} \approx 15.554 \, V \]
3. Determine the Peak Inverse Voltage (PIV):
In a half-wave rectifier, during the negative cycle, the diode is open and the full secondary peak voltage appears across it.
\[ \text{PIV} = V_{s,peak} \approx 15.554 \, V \]
Step 4: Final Answer:
The peak inverse voltage for the diode in this circuit is 15.554 V. This corresponds to option (D).