Step 1: Understanding Full-Wave Rectification In an AC supply, the input signal is sinusoidal with a fundamental frequency \( f_{\text{in}} \). A full-wave rectifier converts both halves of the AC waveform into positive cycles. This means that for each cycle of the input signal, the rectified output completes two cycles.
Step 2: Determining the Ripple Frequency For a full-wave rectifier, the output frequency is given by: \[ f_{\text{ripple}} = 2 f_{\text{input}} \] Given: \[ f_{\text{input}} = 50 \text{ Hz} \] \[ f_{\text{ripple}} = 2 \times 50 = 100 \text{ Hz} \]
Step 3: Evaluating the Options - 50 Hz (Incorrect): This is the input AC frequency, but in a full-wave rectifier, the output frequency doubles.
- 70.7 Hz (Incorrect): This value is incorrect as it does not follow the rectification frequency relation.
- 100 Hz (Correct): This is the correct ripple frequency as per the full-wave rectification principle.
- 25 Hz (Incorrect): This is an unrelated frequency and does not match the rectification formula.
Step 4: Conclusion Thus, the fundamental frequency in the ripple output of a full-wave rectifier operating at 50 Hz is \( 100 \) Hz.
LIST I SCR Rating | LIST II Protective element | ||
A. | di/dt limit | I. | Snubber |
B. | dv/dt limit | II. | Heat Sink |
C. | i2t limit | III. | Series Reactor |
D. | Junction Temperature Limit | IV. | Fuse |
LIST I 1-\(\varnothing\) rectifier topology feeding resistive load | LIST II Output Voltage | ||
A. | Controlled half wave | I. | \(\frac{2V peak}{\pi} cos\ a\) |
B. | Semi-controlled | II. | \(\frac{V peak}{\pi}\) |
C. | Controlled full wave | III. | \(\frac{V peak}{\pi} (1+cos\ a)\) |
D. | Uncontrolled-half wave | IV. | \(\frac{V peak}{2\pi}(1+ cos\ a)\) |