Amplification Classes
- Matheus Antunes

- Nov 12
- 3 min read
My deep dive into the world of amplification began with a genuine curiosity about what makes a studio monitor work. What seemed like a mere detail ended up becoming a determining factor (among others) in the investment strategies for my own business. Realizing the impact this knowledge had on my decisions, I decided to share this technical insight with my industry colleagues to help demystify our tools of the trade.
Audio Amplification
Audio amplification is a constant search for the balance between signal purity and energy efficiency and when we look inside the equipment we find a fascinating story about how we manipulate electricity to create music. Over the decades engineers have developed different operating classes to solve thermal and acoustic problems and each of them brings a unique approach to the task of transforming a weak electrical signal into a force capable of moving a loudspeaker.
The Linear Foundation and the Purity of Class A
It all starts with Class A which is considered by many purists as the gold standard of fidelity. In this configuration the output devices conduct electricity during the entire sound wave cycle and this means the transistors are always on and operating in their most linear region. The great advantage here is the total absence of crossover distortion which is that small error that occurs when the signal passes from one transistor to another. However this purity comes at a high thermal cost because Class A wastes a huge amount of energy in the form of heat even when there is no music playing and this requires large and heavy heat sinks to maintain stable operation.
The Quest for Efficiency with Classes B and AB
To solve the problem of excessive heat Class B emerged utilizing a configuration known as Push-Pull where one transistor handles the positive part of the wave and another the negative part. Although this drastically increases efficiency the moment of switching between transistors generates the dreaded crossover distortion which sounds harsh and unpleasant to our ears. The elegant solution to this dilemma was the creation of Class AB which became the industry standard for many years. Class AB introduces a small bias voltage that keeps both transistors slightly turned on at the crossover point and this eliminates the audible distortion of Class B while maintaining an efficiency far superior to that of Class A.
The Switching Revolution and Class D
Contrary to what many think the letter D does not mean digital but represents the next topology in the historical sequence. Class D amplifiers operate in a radically different way as their transistors function as high-speed switches that turn on and off thousands of times per second. Through a technique called Pulse Width Modulation or PWM the audio signal is encoded in the width of these pulses and then reconstructed by a filter at the output. The thermal efficiency here is extraordinary and exceeds ninety percent which allows very small amplifiers to deliver gigantic power with minimal heat dissipation. Although early versions had problems with high frequencies modern Class D designs rival the sound quality of the best linear implementations.
Intelligent Power Management with Classes G and H
When we enter the territory of high professional power efficiency becomes critical and this is where Classes G and H shine. Class G uses multiple fixed voltage rails and the amplifier automatically switches to a higher voltage rail only when the musical signal demands a power peak. Class H takes this concept a step further by continuously modulating the power supply voltage so that it tracks the audio signal remaining just slightly above what is necessary. The result is an amplifier that runs cool like a Class D but maintains the linear output topology of a Class AB ensuring reliability in large sound systems.
Final Considerations on Amplification
The diversity of amplification classes demonstrates that there is no single perfect solution for all scenarios but rather the right tool for each application. While Class A continues to be revered in critical listening environments where heat and weight are not issues Classes D and H have allowed high-power sound to become portable and accessible. The choice of the ideal topology always depends on the delicate balance between sound fidelity, energy efficiency, physical size and cost and understanding these differences is fundamental for any professional or enthusiast who wishes to extract the best possible performance from their audio system.
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