When people refer to "amplifiers," they're usually talking about stereo components or musical equipment. But this is only a small representation of the spectrum of audio amplifiers. There are actually amplifiers all around us. You'll find them in televisions, computers, portable CD players and most other devices that use a speaker to produce sound.
Now, we'll see what amplifiers do and how they do it. Amplifiers can be very complex devices, with hundreds of tiny pieces, but the basic concept behind them is pretty simple. You can get get a clear picture of how an amplifier works by examining the most basic components.
Electronic sound equipment works the same basic way. It represents sound as a varying electric current. Broadly speaking, there are three steps in this sort of sound reproduction:
Sound waves move a microphone diaphragm back and forth, and the microphone translates this movement into an electrical signal. The electrical signal fluctuates to represent the compressions and rarefactions of the sound wave.
A recorder encodes this electrical signal as a pattern in some sort of medium -- as magnetic impulses on tape, for example, or as grooves in a record.
A player (such as a tape deck) re-interprets this pattern as an electrical signal and uses this electricity to move a speaker cone back and forth. This recreates the air-pressure fluctuations originally recorded by the microphone.
As you can see, all the major components in this system are essentially translators: They take the signal in one form and put it into another. In the end, the sound signal is translated back into its original form, a physical sound wave.
In order to register all of the minute pressure fluctuations in a sound wave, the microphone diaphragm has to be extremely sensitive. This means it is very thin, and moves only a short distance. Consequently, the microphone produces a fairly small electrical current.
This is fine for most of the stages in the process -- it's strong enough for use in the recorder, for example, and it is easily transmitted through wires. But the final step in the process -- pushing the speaker cone back and forth -- is more difficult. To do this, you need to boost the audio signal so it has a larger current while preserving the same pattern of charge fluctuation.
This is the job of the amplifier. It simply produces a more powerful version of the audio signal. In this next section, we'll look at the basic elements in this system.
The input circuit is the electrical audio signal recorded on tape or running in from a microphone. Its load is modifying the output circuit. It applies a varying resistance to the output circuit to recreate the voltage fluctuations of the original audio signal.
The basic concept of an amplifier: A smaller current is used to modify a larger current.
In most amplifiers, this load is too much work for the original audio signal. For this reason, the signal is first boosted by a pre-amplifier, which sends a stronger output signal to the power amplifier. The pre-amplifier works the same basic way as the amplifier: The input circuit applies varying resistance to an output circuit generated by the power supply. Some amplifier systems use several pre-amplifiers to gradually build up to a high-voltage output signal.
So how does the amplifier do this? If you look inside an amplifier for an answer, you'll only find a complex mass of wires and circuitry components. The amplifier needs this elaborate setup to make sure each part of the audio signal is represented correctly and accurately. Hi-fidelity output requires very precise control.
Inside an amplifier, you'll see a mass of electronic components. The central components are the large transistors. The transistors generate a lot of heat, which is dissipated by the heat sink.
All of the pieces in an amplifier are important, but you certainly don't need to examine each one to understand how an amplifier works. There are only a few elements that are crucial to the amplifier's functioning. In the next section, we'll see how these elements come together in a very basic amplifier design.
In pure silicon, all of the silicon atoms bond perfectly to their neighbors, leaving no free electrons to conduct electric current. In doped silicon, additional atoms change the balance, either adding free electrons or creating holes where electrons can go. Electrical charge moves when electrons move from hole to hole, so either one of these additions will make the material more conductive. (See How Semiconductors Work for a full explanation.)
N-type semiconductors are characterized by extra electrons (which have a negative charge). P-type semiconductors have an abundance of extra holes (which have a positive charge).
Let's look at an amplifier built around a basic bipolar-junction transistor. This sort of transistor consists of three semiconductor layers -- in this case, a p-type semiconductor sandwiched between two n-type semiconductors. This structure is best represented as a bar, as shown in the diagram below (the actual design of modern transistors is a little different).
A standard bipolar transistor
The first n-type layer is called the emitter, the p-type layer is called the base and the second n-type layer is called the collector. The output circuit (the circuit that drives the speaker) is connected to electrodes at the transistor's emitter and collector. The input circuit connects to the emitter and the base.
The free electrons in the n-type layers naturally want to fill the holes in the p-type layer. There are many more free electrons than holes, so the holes fill up very quickly. This creates depletion zones at the boundaries between n-type material and p-type material. In a depletion zone, the semiconductor material is returned to its original insulating state -- all the holes are filled, so there are no free electrons or empty spaces for electrons, and charge can't flow. When the depletion zones are thick, very little charge can move from the emitter to the collector, even though there is a strong voltage difference between the two electrodes.
You can change this situation by boosting the voltage on the base electrode. The voltage at this electrode is directly controlled by the input current. When the input current is flowing, the base electrode has a relative positive charge, so it draws electrons toward it from the emitter. This frees up some of the holes, which shrinks the depletion zones. As the depletion zones are reduced, charge can move from the emitter to the collector more easily -- the transistor becomes more conductive. The size of the depletion zones, and therefore the conductivity of the transistor, is determined by the voltage at the base electrode. In this way, the fluctuating input current at the base electrode varies the current output at the collector electrode. This output drives the speaker.
A single transistor like this represents one "stage" of an amplifier. A typical amplifier will have several boosting stages, with the final stage driving the speaker.
In a small amplifier -- the amplifier in a speaker phone, for example -- the final stage might produce only half a watt of power. In a home stereo amplifier, the final stage might produce hundreds of watts. The amplifiers used in outdoor concerts can produce thousands of watts.
The goal of a good amplifier is to cause as little distortion as possible. The final signal driving the speakers should mimic the original input signal as closely as possible, even though it has been boosted several times.
This basic approach can be used to amplify all kinds of things, not just audio signals. Anything that can be carried by an electrical current -- radio and video signals, for example -- can be amplified by similar means. Audio amplifiers seem to catch people's attention more than anything else, however. Sound enthusiasts are fascinated with variations in design that affect power rating, impedance and fidelity, among other specifications.
For much more information on amplifiers, check out the links on the next page.