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CIE AS/A Level Physics 21.2 Rectification and smoothing Study Notes- 2025-2027 Syllabus

CIE AS/A Level Physics 21.2 Rectification and smoothing Study Notes – New Syllabus

CIE AS/A Level Physics 21.2 Rectification and smoothing Study Notes at  IITian Academy  focus on  specific topic and type of questions asked in actual exam. Study Notes focus on AS/A Level Physics latest syllabus with Candidates should be able to:

  1. distinguish graphically between half-wave and full-wave rectification
  2.  explain the use of a single diode for the half-wave rectification of an alternating current
  3. explain the use of four diodes (bridge rectifier) for the full-wave rectification of an alternating current
  4. analyse the effect of a single capacitor in smoothing, including the effect of the values of capacitance and the load resistance

AS/A Level Physics Study Notes- All Topics

Half-Wave and Full-Wave Rectification 

Rectification is the process of converting an alternating current (AC) signal into a unidirectional (DC) signal. The easiest way to distinguish between half-wave and full-wave rectification is by examining their voltage–time graphs.

Half-Wave Rectification

  • Only one half-cycle (usually the positive half) of the AC waveform is allowed through.
  • The diode blocks the negative half-cycle completely → output voltage is zero during negative cycle.
  • Graph shows:
    •  Positive sine pulses  
    • Flat line (zero output) during each negative half-cycle

 

Full-Wave Rectification

  • Both halves of the AC waveform are used.
  • The negative half-cycle is inverted to become positive.
  • Graph shows:
    •  Positive output for both halves  
    • Twice as many pulses per cycle compared to half-wave

Graphical Comparison (Conceptual Description)

  • Half-wave:  \( \mathrm{V(t) = V_0 \sin(\omega t)} \) for positive half  \( \mathrm{V(t) = 0} \) for negative half  → Output has gaps.
  • Full-wave:  \( \mathrm{V(t) = |V_0 \sin(\omega t)|} \)  → No gaps; negative half is flipped.

Example

A student observes a rectified AC signal on an oscilloscope. The trace shows positive pulses with flat zero regions between them. Identify the type of rectification.

▶️ Answer / Explanation

This waveform shows gaps between pulses → output is zero during half the cycle.

Therefore, it is half-wave rectification.

Example

An oscilloscope displays a waveform where all cycles of the sine wave appear above the time axis, with no zero gaps. Explain what type of rectification is occurring and why.

▶️ Answer / Explanation

All negative cycles have been inverted into positive cycles, and there are no zero intervals.

This is characteristic of full-wave rectification, where a diode bridge or two diodes in a centre-tap transformer invert the negative half-cycle.

Example

A rectified waveform has twice the frequency of the original AC supply. The waveform is always positive and has no gaps. Identify the type of rectification and justify your answer graphically.

▶️ Answer / Explanation

The doubling of frequency indicates that every half-cycle (positive and negative) produces a pulse.

Since there are no zero intervals and all pulses are above the axis, the waveform is:

Full-wave rectification

Graphically, full-wave rectification produces twice as many peaks per period as the original AC input because both halves of the sine wave are used.

Use of a Single Diode for Half-Wave Rectification

A single diode can be used to convert an alternating current (AC) into a unidirectional (DC) output. This process is known as half-wave rectification.

How It Works:

  • A diode conducts current only when it is forward biased (positive on the anode, negative on the cathode).
  • During the positive half-cycle of the AC supply, the diode is forward biased → current flows → output follows the positive sine wave.
  • During the negative half-cycle, the diode is reverse biased → no current flows → output is zero.

Result:

Only the positive half of the AC waveform appears at the output. The negative half is completely blocked → producing half-wave rectification.

Graphically:

  • Input: full sine wave (positive + negative halves).
  • Output: positive “humps” separated by flat zero intervals.

Advantages:

  • Simple circuit (only one diode).
  • Low cost.

Disadvantages:

  • Poor efficiency — half the input power is lost.
  • Large ripple (output not smooth).

Example

Explain why a single diode gives zero output during the negative half-cycle of an AC input.

▶️ Answer / Explanation

During the negative half-cycle, the anode of the diode becomes negative relative to the cathode. This reverse biases the diode, preventing current flow. Therefore, the output voltage is zero.

Example

A single diode is connected to an AC source. Describe the shape of the output waveform and explain why it appears this way.

▶️ Answer / Explanation

The output consists of only the positive half-cycles of the sine wave, with zero output in between.

Reason: the diode conducts only when forward biased (positive half-cycle), but blocks the current when reverse biased (negative half-cycle), producing gaps in the waveform.

Example

An AC input has a peak voltage of 12 V. A single diode is used for half-wave rectification. Sketch and describe the output waveform and determine the peak output voltage assuming an ideal diode.

▶️ Answer / Explanation

Shape of output:

  • Positive half-cycles appear unchanged.
  • Negative half-cycles are completely absent (output = 0).
  • Waveform looks like isolated positive humps.

Peak output voltage:

For an ideal diode, no voltage drop occurs → peak output = 12 V.

Output peak = 12 V

Full-Wave Rectification Using a Four-Diode Bridge Rectifier

A bridge rectifier uses four diodes arranged in a specific configuration to convert both halves of an AC waveform into a unidirectional (positive) output. This makes it far more efficient than half-wave rectification.

How the Bridge Rectifier Works

A bridge rectifier has four diodes arranged in a diamond shape. During each half-cycle of the AC input, two of the four diodes conduct while the other two are reverse biased.

Positive Half-Cycle:

  • The top of the AC supply becomes positive relative to the bottom.
  • Diodes D1 and D2 conduct.
  • Current flows through the load in one direction.
  • Diodes D3 and D4 are reverse biased → they block current.

Negative Half-Cycle:

  • The top of the AC supply becomes negative relative to the bottom.
  • Diodes D3 and D4 conduct.
  • Current again flows through the load in the SAME direction.
  • D1 and D2 are now reverse biased → they block current.

Result:

Both halves of the AC input produce a positive output → full-wave rectification.

Graphically:

  • Input: full sine wave
  • Output: all positive humps, no zero intervals
  • Output frequency = twice the input AC frequency

Advantages of the Bridge Rectifier:

  • Uses both halves of AC waveform → higher efficiency
  • No need for a centre-tapped transformer
  • Smoother DC output compared to half-wave

Example

Explain why full-wave rectification produces twice as many output pulses as half-wave rectification.

▶️ Answer / Explanation

In a bridge rectifier, both positive and negative half-cycles are used. The negative half-cycle is inverted to become positive using two of the four diodes. Thus, each cycle produces two pulses → double the number in half-wave rectification.

Example

During the positive half-cycle of an AC supply feeding a bridge rectifier, only two of the diodes conduct. Name them and explain why the others do not conduct.

▶️ Answer / Explanation

During the positive half-cycle, diodes D1 and D2 become forward biased → they conduct.

Diodes D3 and D4 have their cathodes made more positive than their anodes during this part of the cycle → they are reverse biased → they do not conduct.

Example

An AC supply of peak voltage 18 V is connected to a bridge rectifier (ideal diodes). Describe the output waveform and determine the peak output voltage across the load.

▶️ Answer / Explanation

Output waveform:

  • Every positive and negative half-cycle produces a positive pulse.
  • The output voltage never goes negative.
  • Pulses occur twice per AC cycle → doubled frequency.

Peak output voltage:

For ideal diodes, no voltage is lost → peak output = peak input.

\( \mathrm{V_{0,\text{out}} = 18\ V} \)

Peak output = 18 V

Smoothing a Rectified Output Using a Capacitor

After rectification (half-wave or full-wave), the output is still “pulsating DC.” A smoothing capacitor is connected in parallel with the load to reduce the size of these ripples and produce a smoother DC output.

How Smoothing Works:

  • When the rectified voltage increases (during each peak), the capacitor charges up.
  • When the rectified voltage falls (between peaks), the capacitor discharges slowly through the load.
  • This discharge maintains the output voltage → smoothing the waveform.

The result is a DC voltage that still has some ripple, but the variations are much smaller.

Graphically:

  • Without capacitor → sharp peaks and deep valleys.
  • With capacitor → voltage rises to a peak, then falls gradually (exponential discharge), then rises again.
  • The ripple becomes smaller as smoothing improves.

Ripple Voltage:

Ripple depends on how much the capacitor discharges between peaks.

Effect of Capacitance on Smoothing

  • Larger capacitance (large C)
    • Stores more charge  
    • Discharges more slowly  
    • Smoother output (smaller ripple)
  • Smaller capacitance (small C)
    • Holds less charge  
    • Discharges quickly  
    • Larger ripple (poor smoothing)

Summary:

Bigger C → better smoothing.

Effect of Load Resistance on Smoothing

  • High load resistance (large R)  •
    • Small current drawn  
    • Capacitor discharges slowly  
    • Ripple decreases → better smoothing
  • Low load resistance (small R)
    • Large current drawn  
    • Capacitor discharges quickly  
    • Ripple increases → poor smoothing

Summary:

Larger R → better smoothing.

Time Constant and Smoothing

\( \mathrm{\tau = RC} \)

  • Large \( \mathrm{\tau} \) → capacitor discharges slowly → smooth output.
  • Small \( \mathrm{\tau} \) → capacitor discharges quickly → large ripple.

Example

A capacitor is connected across the output of a half-wave rectifier. The output voltage becomes smoother. Explain why the capacitor improves smoothing.

▶️ Answer / Explanation

The capacitor charges during the peak and discharges between peaks, supplying current to the load. This prevents the voltage from dropping to zero, reducing ripple and creating a smoother DC output.

Example

Two smoothing capacitors are tested: \( \mathrm{10\ \mu F} \) and \( \mathrm{470\ \mu F} \). Which gives a smoother output and why?

▶️ Answer / Explanation

The \( \mathrm{470\ \mu F} \) capacitor stores more charge and discharges more slowly, keeping the output voltage high between peaks. Therefore, it produces a much smoother DC output with less ripple.

Example

A full-wave rectifier outputs pulses at twice the mains frequency. The smoothing capacitor is \( \mathrm{220\ \mu F} \). Explain how decreasing the load resistance affects the ripple voltage.

▶️ Answer / Explanation

When the load resistance decreases, a larger current is drawn. The capacitor discharges more rapidly between the rectified peaks.

This causes the minimum voltage during each cycle to drop further → increasing the ripple voltage.

Because:

\( \mathrm{\tau = RC} \) decreases → faster discharge → poorer smoothing.

Thus, lower R → higher ripple → less effective smoothing.

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