When it comes to amplifier operation classes, not all hi-fi enthusiasts really understand what these classes mean in practice. We hear “Class A”, “Class D”, or “hybrid” thrown around in reviews and forums, often with a lot of strong opinions attached. In this article, I’ll cover solid-state (transistor) Class A, Class AB, Class D, and hybrid amplifiers, and explain them in a way that doesn’t require an electronics degree.
The aim is simple: help you understand how these amplifier classes behave, how they tend to sound, and which one might make sense for your system and listening habits. I’ll include simple pros and cons for each, plus some honest recommendations based on real-world use rather than marketing hype.
I’ll start with the most common and widely used amplifier class: Class AB. This has been, and still is, the most sensible and well-balanced way to run a solid-state amplifier. I won’t go into circuit theory, but rather how it behaves and why it became the reference point. To make the other classes easier to understand, I’ll compare everything back to the mighty Class AB.
Class AB is the workhorse of hi-fi. Most classic and modern solid-state amplifiers use it because it offers a very good compromise between sound quality, efficiency, heat, size, and cost. In simple terms, Class AB amplifiers keep their output transistors just slightly turned on all the time. This avoids obvious switching artefacts, but doesn’t waste huge amounts of power when there is no music playing.
In normal listening conditions, a well-designed Class AB amplifier is clean, controlled, punchy, and reliable. It can deliver real power without becoming impractically large or hot, and it works with a wide range of speakers. This is why so many respected designs from the 70s through to today are Class AB.
The good: good sound quality, good efficiency, manageable heat, reasonable size and cost, and excellent reliability.
The bad: it doesn’t quite have the purity or “magic” of Class A, and badly designed examples can suffer from crossover distortion, although this is largely a solved problem in decent designs.
For most people, most of the time, Class AB remains the best all-round choice.
Class A is the dream of many audiophiles, including me. It’s the closest solid-state technology ever got to valves (or tubes, for US readers), although valves deserve a separate article of their own. Conceptually, Class A is not a completely different animal from Class AB, it’s more like running the same engine in a very different way.
Imagine a car engine idling, and then you press the accelerator when you want power. That’s Class AB. Now imagine the same engine running flat-out all the time, whether you’re moving or not. That’s Class A. In a car, this would be madness, but in an amplifier, this behaviour has real sonic advantages.
In a Class A amplifier, the output transistors are always conducting large currents. A modest 20 W Class A amplifier can easily run 1.5–2 amps continuously through the output stage. When the music signal arrives, nothing needs to “wake up” or switch on. The devices are already fully active. This eliminates switching delays, reduces certain types of distortion, and keeps the power supply under a constant load.
The result, when done properly, can be stunning. Effortless midrange, smooth treble, a sense of flow and realism that many listeners find addictive.
The good: exceptional sound quality, especially at low and medium listening levels; very natural and fluid presentation.
The bad: terrible efficiency, lots of heat, very heavy and expensive hardware. A small Class A amplifier might draw 50–80 W continuously just to deliver 20 W of audio power, with the rest turning into heat. This means huge heatsinks, big transformers, and massive capacitor banks.
Class A only really makes sense once the rest of your system is already at a high level. You need speakers that can show the difference, space to deal with the heat, and acceptance that you’re paying for sound quality rather than practicality.
Class D is the new kid on the block, although in reality it has been around for decades. What’s changed recently is that it has finally grown up. Early Class D amplifiers were efficient but often sounded rough or artificial. Modern designs are a very different story.
A simple way to think about Class D is not “digital amplification” (despite the name), but a very fast switching power amplifier. Instead of amplifying a smooth, linear signal like Class AB or A, the output transistors switch fully on and fully off at extremely high speeds. The audio signal is encoded into these on/off patterns, then reconstructed back into music by an output filter.
Because the transistors are either fully on or fully off, they waste very little power. Efficiencies of 85–95% are common, compared to 30–40% for Class A and around 50–70% for Class AB.
The good: very high efficiency, compact size, low heat, lighter weight, and the ability to deliver lots of power cheaply. Modern Class D can sound excellent, with tight bass and very low distortion.
The bad: design complexity, sensitivity to layout and power supply quality, and a sound that some still find a little “matter of fact” compared to Class A or good AB. Poor implementations still exist.
Class D makes huge sense for high-power systems, subwoofers, active speakers, and modern compact hi-fi. It’s no longer the compromise it once was, but it still rewards careful design.
Class T is often mentioned alongside Class D, and for good reason: technically, it is a variation of Class D rather than a completely separate class. Class T was popularised by Tripath chips in the early 2000s and used a proprietary control method that adjusted the switching behaviour in a more “analogue-like” way. The result was surprisingly musical sound from very small, efficient amplifiers, often better than early Class D designs. The downside is that Tripath no longer exists, so Class T is mostly of historical interest today, but many of those small amps still have a loyal following.
Class H is less talked about in home hi-fi, but it is very common in professional and high-power amplifiers. It is essentially an evolution of Class AB that uses multiple power supply voltage rails. At low listening levels the amplifier runs on lower voltages to reduce heat and waste, and as more power is needed it switches to higher voltage rails. This improves efficiency without fully abandoning linear amplification. When done well, Class H can sound very similar to Class AB, but with better efficiency at high power levels.
Hybrids sit somewhere between these worlds. The most common hybrid approach uses valve pre-amplification combined with a solid-state power amplifier, usually Class AB or Class D. The idea is to blend the harmonic richness and character of valves with the control, power, and reliability of transistors.
Some hybrids also bias their solid-state output stages closer to Class A at low levels, sliding into Class AB as power demand increases. Others use Class D power stages with valve input stages to add a bit of flavour.
The good: flexibility, character, often a pleasing balance of warmth and control.
The bad: complexity, cost, and sometimes neither side fully delivers if the design is not well-balanced.
In terms of recommendations, Class AB remains the safest and most universally sensible choice. If you want maximum sound quality and are happy to live with heat, size, and cost, Class A can be magical. If efficiency, compactness, or high power matter, modern Class D deserves serious consideration. Hybrids are for those who enjoy experimentation and character, and who value system matching over purity.
There is no single “best” class, only the best choice for your system, your room, and how you listen.
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