Comparison

Class A vs Class B Amplifier

The LM386 audio amplifier IC operates in class AB — a concession to the fact that pure class A would burn most of the supply power as heat in the output transistor even with no audio signal. A class A amplifier is ON for the full 360° of the input cycle; a class B transistor conducts for only 180°. That single difference in conduction angle drives every trade-off: efficiency, distortion, thermal design, and cost.

EEE, ECE, EI

Side-by-side comparison

ParameterClass AClass B Amplifier
Conduction angle360° (full cycle)180° (half cycle each transistor in push-pull)
Quiescent current I_QHigh — transistor biased at midpoint continuouslyNear zero — transistors biased at cutoff
Maximum efficiency (η)25% (resistive load), 50% (transformer-coupled)78.5% (theoretical maximum)
Distortion typeLow harmonic distortion; linear operationCrossover distortion at 0 V transition
THD (typical)< 0.1% (well-biased)5–10% (without correction)
Heat dissipationHigh even at idle (P = V_CC × I_Q)Low at idle; rises with signal
Biasing requirementFixed DC bias at Q-point midway on load lineV_BE = 0 (or near 0) — transistors at cutoff
Output stage transistorsSingle transistor (or complementary pair biased ON)Complementary NPN+PNP pair, each active 180°
Typical applicationLow-power precision audio, small signal stagesHigh-power audio, RF power amplifiers (not audio)
Example circuitBC547 single-ended preamp; LM1875 biased class ATDA2030 push-pull; discrete 2N3055+MJ2955 pair

Key differences

Class A's 25% maximum efficiency (resistive load) means three-quarters of supply power is wasted as heat — a 10 W output class A amp dissipates at least 30 W in the transistor even with no music playing. Class B's 78.5% theoretical efficiency makes it attractive for battery-powered and high-power applications, but crossover distortion — where neither transistor is active during the zero-crossing — introduces THD of 5–10% without correction. This distortion is audible in speakers; the 2N3055/MJ2955 push-pull pair used in textbook class B circuits sounds noticeably harsh on voice. For the same 10 W output, class B dissipates only about 3 W in the transistors. There is no configuration where class A efficiency equals class B, and no class B without crossover distortion unless you add a forward bias — which turns it into class AB.

When to use Class A

Use class A when linearity and low distortion matter more than efficiency — typically in small-signal preamp stages, headphone amplifiers, and precision measurement amplifiers. A single BC547 in a class A common-emitter stage with a 4.7 kΩ collector load delivers < 0.1% THD at 1 kHz.

When to use Class B Amplifier

Use class B when you need to deliver high power efficiently and can accept correction for crossover distortion through signal processing or a small forward bias. A 2N3055/MJ2955 complementary push-pull pair driving an 8 Ω speaker from ±30 V supplies delivers 50 W at 78% efficiency — impossible with class A at that power level.

Recommendation

For any audio output stage above 1 W, choose class B or class AB — efficiency wins. For input stages and low-power precision amplifiers, choose class A — the distortion figure is decisive. No real design uses pure class B; but understanding it is essential because class AB is simply class B with a small corrective bias added.

Exam tip: Examiners ask for derivations of maximum efficiency for both classes — prove η_max = 25% for class A (P_out / P_DC = V_m²/2R_L ÷ V_CC²/R_L, where V_m = V_CC/2) and η_max = π/4 ≈ 78.5% for class B using the push-pull analysis.

Interview tip: Interviewers expect you to explain crossover distortion in class B physically — not just that it exists, but that both transistors are simultaneously off during zero crossing because V_BE < 0.6 V for each, creating a dead zone that causes audible distortion in the output waveform.

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