Mean a.c. power and half-wave rectification

Key idea: H2 Physics lessons on drift velocity, electrical energy, sinusoidal supplies and half-wave rectification.

  • GCE A-Level H2 Physics 2027

Learn the idea

Big question: How can an alternating supply deliver steady heating or one-way current?

For a resistive load, mean power is VrmsIrms = I²rmsR. A diode in series produces half-wave rectification by blocking one half-cycle, so current becomes unidirectional but pulsating. Distinguish the input a.c. waveform from the load output and account for diode orientation.

Calculate mean power with r.m.s. values

For a pure resistor, instantaneous power is p = vi = i²R. Averaging over a sine-wave cycle gives Pmean = I_rms²R = V_rms²/R = V_rms I_rms. Peak values may be used only after the correct factor of one half is included.

Voltage and current are in phase for a resistor, so both reverse together and their product stays positive. This lesson does not assume the same expression without care for reactive components.

Check your understanding: A 6.0 V r.m.s. supply is connected to 12 Ω. Find mean power.

P = V_rms²/R = 36/12 = 3.0 W.

Follow the conducting path through a diode

A diode conducts mainly in one direction. In a half-wave rectifier it passes one half-cycle and blocks the other, producing a pulsating but unidirectional load current. Reversing the diode passes the opposite half-cycles.

Draw input and output on aligned time axes. The output is not a smaller sine wave: the blocked intervals sit at zero in the ideal-diode model. Rectification changes direction pattern; smoothing would require additional components and is a separate idea.

Check your understanding: Does half-wave rectification produce direct current?

It produces unidirectional, pulsating current. It is not constant unless further smoothing is used.

Ideal single-diode half-wave rectifierA sinusoidal alternating-voltage source is connected in series with an ideal diode and load resistor. The diode anode is on the source side and its cathode is on the load side. An output voltmeter is connected across the load with positive polarity at the top. Arrows show clockwise conventional current during the conducting half-cycle; notes state that the opposite half-cycle is blocked.Single diode selects one half-cyclesinusoidal inputvᵢₙ changes polarityideal diodeanodecathodeconventional IloadRV+−Vₒᵤₜ across R+−conducting half-cycle:top terminal positiveForward biased: diode conductsI flows clockwise; Vₒᵤₜ is a positive pulse.Reverse biased: diode blocksIdeal model: I = 0 and Vₒᵤₜ = 0.
Scroll diagram horizontally to read all labels.
When the source makes the diode's anode positive relative to its cathode, conventional current passes through the load and Vout is positive. On the opposite half-cycle the ideal diode blocks, so I = 0 and Vout = 0.

Key ideas to keep

  • Mean voltage and r.m.s. voltage are different quantities.
  • Half-wave rectification uses only alternate half-cycles.
  • Reversing the diode reverses which half-cycle appears across the load.

Worked example

Derive mean resistor power before rectifying the waveform

Question: Show why a sinusoidal current produces mean power equal to half its peak power in a resistor.

  1. Step 1: Write instantaneous power

    Why: Resistor power depends on current squared.

    Working: With i = I₀sinωt, p = i²R = I₀²R sin²ωt.

  2. Step 2: Average over one cycle

    Why: The mean of sin² over a complete cycle is one half.

    Working: Pmean = ½I₀²R = I_rms²R.

  3. Step 3: Compare with the peak

    Why: Peak power occurs when sin²ωt = 1.

    Working: Pmax = I₀²R, so Pmean = Pmax/2.

Answer: With i = I₀ sin ωt, p = i²R = I₀²R sin²ωt. The mean of sin² over a complete cycle is ½, so ⟨P⟩ = ½I₀²R = Iᵣₘₛ²R and Pmax = I₀²R.

Check: Power never becomes negative even though current reverses.

Practise with support

Try this

Peak power in a sinusoidally driven resistor is 72 W. State mean power and explain why a single diode does not produce steady d.c.

Hint: Separate direction from constancy.

Check your answer

Mean power is 36 W. The diode blocks alternate half-cycles, so the output is unidirectional but falls to zero for half of every cycle.

Practise independently

Your turn

Sketch verbally the input, diode state and load output throughout one cycle of half-wave rectification.

Check your answer

During the forward-biased half-cycle the diode conducts and the load follows that half-sinusoid. During the reverse-biased half-cycle it blocks and load current is zero. The result is one same-polarity pulse per input cycle, not smooth d.c.

Common mistakes

Common mistake

Mean power is found by averaging current before squaring it.

What is wrong with this reasoning?

Show better thinking

Instantaneous resistive power is i²R; average sin² over the cycle, giving one half.

Common mistake

One diode converts a.c. into steady d.c.

What is wrong with this reasoning?

Show better thinking

One diode produces a pulsating half-wave output; smoothing would require additional components.

Exam guidance

Sketch input and output on aligned time axes and label the conducting half-cycle.

Exam-style practice [5 marks]

A resistor has peak sinusoidal power 200 W. Find mean power and explain how one diode changes a full sinusoid.

Plan before you answer

  • Use the sine-wave mean-power relation.
  • Trace the diode during both half-cycles.
  • Describe output direction and variation separately.
Mark your answer and compare the model

Marking points

Tick each point only if your answer states it clearly.

Model answer

Mean power is 100 W because ⟨sin²⟩ = ½. A single diode conducts for one half-cycle and blocks the other, giving a pulsating half-wave output with one pulse per cycle.

Check what stayed with you

Recall question

State one difference between half-wave rectified output and steady d.c., and give its pulse frequency for a 60 Hz input.

Check the answer

Half-wave output varies from zero to a peak rather than remaining constant. It has one pulse per input cycle, so its pulse frequency is 60 Hz.

Try this next

Use the longer mixed questions to connect the ideas, calculations and diagrams from this topic.

Open Current Electricity structured practice

Syllabus and review details

This lesson covers the listed H2 Physics 9478 outcomes. Topic 15 states no explicit exclusions. q in I = nAvq is treated as carrier-charge magnitude when calculating current magnitude; electron drift is opposite conventional current. E.m.f. is energy supplied per unit charge, while p.d. is energy transferred from electrical form per unit charge. The peak/√2 and half-maximum-power results are restricted to sinusoidal waveforms and a resistive load; a single ideal diode gives unsmoothed half-wave rectification.

  • GCE A-Level H2 PhysicsTopic 15(h) / Topic 15(j) · 2027Checked against the syllabus · partial topic coverageOfficial 9478 syllabus
Course and syllabus information
Course
GCE A-Level H2 Physics
Edition
GCE A-Level H2 Physics 2027