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Audio amplifier

 
Sci-Tech Encyclopedia: Audio amplifier

An electronic circuit for amplification of signals within or somewhat beyond the audio frequency range (generally regarded as 20 to 20,000 Hz). Audio amplifiers may function as voltage amplifiers (sometimes called preamplifiers), power amplifiers, or both. In the last case, they are often called integrated amplifiers. See also Power amplifier.

The function of integrated amplifiers (or of the combination of separate voltage amplifiers and power amplifiers used together) is to amplify a weak signal, such as from a microphone, phonograph pickup, tape player, radio tuner, or compact disc player, to a level capable of driving a loudspeaker or other type of transducer such as headphones at the desired sound level. Power amplifiers may have power ratings ranging from less than 1 W to several hundreds of watts. Stereo amplifiers consist of two identical, but electrically independent, amplifier circuits housed in a single chassis, often sharing a common power supply. Audio amplifiers are commonly constructed with solid-state devices (transistors and integrated circuits), although some amplifiers using vacuum tubes as the active, amplifying devices are still manufactured. See also Amplifier; Integrated circuits; Loudspeaker; Transistor; Vacuum tube.

The ideal amplifier delivers an output signal that, aside from its higher power level, is identical in relative spectral content to the input signal. Normally, various forms of distortion are generated by the amplifier, such as harmonic distortion (multiples of the desired signal frequency), intermodulation distortion (spurious sum or difference frequencies created when multiple tones are applied to the amplifier simultaneously, as in the case of music or speech amplification), and transient intermodulation distortion (caused by rapid fluctuations of the input signal level). All forms of distortion are measured as percentages of the desired signal amplitude. Generally, distortion levels of under 1% or 0.5% are considered to be low enough for high-fidelity applications. See also Fidelity.

Other parameters used to define an amplifier's characteristics include frequency response and signal-to-noise ratio (S/N). The frequency response is the range of frequencies that the amplifier can handle, usually quoted with a tolerance in decibels, for example: “frequency response: 20 to 20,000 Hz, ±0.5 dB.” Signal-to-noise ratio, also quoted in decibels, is indicative of the amount of residual noise generated by the amplifier itself, as compared with the desired output signal level. Signal-to-noise levels greater than 70 dB are generally considered to be acceptable, although some amplifiers offer much better values. See also Response; Signal-to-noise ratio.


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Intelligence Encyclopedia: Audio Amplifiers
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Any electronic device that increases the power of an electrical signal whose vibrations are confined to the audio frequency range—the range that can be perceived by the human ear—is an audio amplifier. All devices that transmit, record, or otherwise electronically process voice signals employ audio amplifiers. Voice-recognition or voice-synthesis systems, communications or eavesdropping devices, hearing aids, entertainment systems, talking toys, are examples of devices containing audio amplifiers.

The need for amplification. Acoustic or sound waves are longitudinal pressure waves (i.e., waves that cause molecules to oscillate along the wave's line of travel rather than across it) in air, water, or any other medium. A sound is said to be in the audio frequency range if it is not too high or low in frequency to be heard by the human ear. Audio sound waves may be converted by microphones into electrical signals for analysis, transmission, or recording. Electrical signals can also be converted by speakers into audible sound waves. Microphones and speakers are both transducers, that is, devices that convert energy from one form (e.g., electrical) into another (e.g., acoustic) or vice versa. Audio amplifiers are required with both microphones and speakers.

Input amplification. Amplification of the signal produced by a microphone—often termed preamplification—is necessary because the electrical signal that can be derived directly from sound waves impinging on a microphone is weak (i.e., on the order of .01 V or less; for eavesdropping applications, much less). Input signals of such low amplitude must be amplified before they can be processed in either analog or digital circuits.

In analog circuits—circuits that process smoothlyvarying electrical quantities—there is a always a certain amount of random electrical activity or "noise." This noise is mixed with any information signal processed by the circuit, corrupting it. Amplifying a weak input, such as that from a microphone, before it mingles with circuit noise makes the noise problem manageable. Furthermore, all analog circuits that lack amplification (passive filters, transmission lines, etc.) experience signal loss; that is, they dissipate energy. A weak signal fed into a circuit that does not contain amplification will, therefore, quickly disappear, making amplification necessary in most analog circuits. Finally, amplification provides electronic isolation between the signal being amplified and the result of the amplification process; among other gains, this simplifies the circuit-design process.

If an audio signal is to be processed using digital circuitry (as is often the case today), a digital signal (i.e., on-off, high-low signal that can represent signal magnitudes symbolically) must be derived from the analog input. This conversion is performed by a device termed an analog-to-digital converter. For reasons ultimately deriving from the atomic properties of semiconductors, a typical analog-to-digital converter requires an analog input signal with an amplitude variation on the order of several volts. A low voltage signal must therefore usually be amplified before being digitized.

Output amplification. Wherever human ears are the ultimate destination of a signal it is necessary to drive a physical sound-making device at the output. Here audio amplification is needed for a reason complementary to that which applies at the input: the signal power needed to drive an output device (e.g., speaker or headphones) is greater than that conveyed by the signals processed throughout the circuitry of a typical electronic device, whether analog or digital. An audio amplifier is thus found at the output as well as at the input of almost every system handling signals in the audio range.

Applications. The number of audio amplifier designs that have been produced over the last century is probably in the hundreds of thousands. Such devices are a ubiquitous feature of modern life, and are found in computers, telephones, radios, high-fidelity audio systems, all military voice-communication systems, many appliances, and even toys.

Audio amplifiers can be miniaturized for placement in headsets, mobile phones. In applications where small size is at a premium, as in hearing aides and espionage applications (bugs and "wires"), they may be ultraminiaturized. At the high-power end, audio amplification drives public-address systems, speaker systems, and (potentially) weapons. Research is being conducted by several countries, including Russia and the U.S. (through its Low Collateral Damage Munitions Program), into the use of highly amplified sound as a weapon; frequencies in the infrasonic, audio, and ultrasonic ranges are all being considered for use against human beings. Though acoustic weapons are sometimes assumed to always be in the nonlethal category, sound can be irritating, painful, or fatal, depending on its intensity and on the efficiency with which its energy is coupled to the body.

Loud music has repeatedly been used as a psychological weapon in siege situations (e.g., by the U.S. Army against former Panamanian dictator Manuel Noriega in 1989, by cult leader David Koresh against police in 1993, and by Peruvian police during the hostage crisis at the Japanese Embassy in 1997) and as an instrument of torture. Specially-designed acoustic weapons can induce, among other effects, vomiting, choking, spasms, incontinence, thermal burns, intolerable sensations in the chest, injury to internal organs, and hearing damage. The latter is considered a serious drawback in antipersonnel applications, as hearing loss caused by intense sound is often partly or wholly permanent. Like laser weapons designed to blind (which have been outlawed by recent international agreement), acoustic weapons designed to deafen would violate international humanitarian law. Further, they would be vulnerable to obvious countermeasures, such as earplugs. Indeed, some scientists are skeptical about the possibility of developing reliable, affordable weapons of any kind from sound. However, research and development are proceeding. Military and security applications of high-intensity sound currently under development in the U.S. or elsewhere include the following

1. A device projecting "acoustic bullets," baseball-sized pulses of low-frequency (10-Hz) sound over distances of hundreds of yards, scalable in intensity from painful to lethal.

2. Multisensory grenades emitting disorienting light flashes, painfully loud sounds, and possibly disagreeable odors.

3. A ship-mounted system to disable crewmembers of nearby vessels (e.g., prior to boarding by Coast Guard personnel).

4. The "directed-stick radiator," an audio frequency, battery-powered weapon that could be clipped to a rifle. It fires acoustic bullets with a range in the tens of feet.

5. A helicopter-mounted nonlethal weapon emitting painfully loud sound in the audible range, with a reported (but unlikely) range of 1.2–6 miles (2–10 km).

6. Acoustic-beam weapons designed to cause discomfort: intended for embassy defense, denial of access to sensitive facilities, crowd control, and other miscellaneous antipersonnel uses.

It is unlikely that such devices will see widespread application or that, if they do, they will replace ordinary lethal weapons such as firearms. Due to the tendency of sound waves to diffuse with distance, the unpredictability of their effects on individual persons at sub-lethal levels, and the extremely high power requirements (megawatt range) for lethal levels, acoustic weapons are likely to remain a military curiosity. Audio amplification will thus remain ubiquitous in communications devices and rare in weaponry.

Further Reading

Books

Jones, Dwight V., and Richard F. Shea. Transistor Audio Amplifiers. New York: John Wiley & Sons, 1968.

Periodicals

Altmann, Jürgen. "Acoustic Weapons-A Prospective Assessment." Science and Global Security no. 9 (2001): 165–244.

Electronic

Roxana, Tiron. "Acoustic-Energy Research Hits Sour Note." National Defense Magazine. August 21, 2001. <http://www.nationaldefensemagazine.org/article.cfm?Id=746> (December 13, 2002).

WordNet: audio amplifier
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Note: click on a word meaning below to see its connections and related words.

The noun has one meaning:

Meaning #1: an amplifier that increases the amplitude of reproduced sound


Wikipedia: Audio amplifier
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Mission Cyrus 1 Hi Fi integrated audio amplifier

An audio amplifier is an electronic amplifier that amplifies low-power audio signals (signals composed primarily of frequencies between 20 hertz to 20,000 hertz, the human range of hearing) to a level suitable for driving loudspeakers and is the final stage in a typical audio playback chain.

The preceding stages in such a chain are low power audio amplifiers which perform tasks like pre-amplification, equalization, tone control, mixing/effects, or audio sources like record players, CD players, and cassette players. Most audio amplifiers require these low-level inputs to adhere to line levels.

While the input signal to an audio amplifier may measure only a few hundred microwatts, its output may be tens, hundreds, or thousands of watts.

Contents

History

Three audio amplifiers

The audio amplifier was invented in 1909 by Lee De Forest when he invented the triode vacuum tube. The triode was a three terminal device with a control grid that can modulate the flow of electrons from the filament to the plate. The triode vacuum amplifier was used to make the first AM radio.[1]

Early audio amplifiers were based on vacuum tubes (also known as valves), and some of these achieved notably high quality (e.g., the Williamson amplifier of 1947-9). Most modern audio amplifiers are based on solid state devices (transistors such as BJTs, FETs and MOSFETs), but there are still some who prefer tube-based amplifiers, due to a perceived 'warmer' valve sound. Audio amplifiers based on transistors became practical with the wide availability of inexpensive transistors in the late 1960s.

Design parameters

Key design parameters for audio amplifiers are frequency response, gain, noise, and distortion. These are interdependent; increasing gain often leads to undesirable increases in noise and distortion. While negative feedback actually reduces the gain, it also reduces distortion. Most audio amplifiers are linear amplifiers operating in class AB.

Filters and preamplifiers

Historically, the majority of commercial audio preamplifiers made had complex filter circuits for equalization and tone adjustment, due to the far from ideal quality of recordings, playback technology, and speakers of the day.

Using today's high quality (often digital) source material, speakers, etc., such filter circuits are usually not needed. Audiophiles generally agree that filter circuits are to be avoided wherever possible. Today's audiophile amplifiers do not have tone controls or filters.

Since modern digital devices, including CD and DVD players, radio receivers and tape decks already provide a "flat" signal at line level, the preamp. is not needed other than as volume control. One alternative to a separate preamp. is to simply use passive volume and switching controls, sometimes integrated into a power amp. to form an "integrated" amplifier.

Further developments in amplifier design

For some years following the introduction of solid state amplifiers, their perceived sound did not have the excellent audio quality of the best valve amplifiers (see valve audio amplifier). This led audiophiles to believe that valve sound had an intrinsic quality due to the vacuum tube technology itself. In 1972, Matti Otala demonstrated the origin of a previously unobserved form of distortion: transitory intermodulation distortion (TIM), also called slew rate distortion. TIM distortion was found to occur during very rapid increases in amplifier output voltage.[2] TIM did not appear at steady state sine tone measurements, helping to hide it from design engineers prior to 1972. Problems with TIM distortion stem from reduced open loop frequency response of solid state amplifiers. Further works of Otala and other authors found the solution for TIM distortion, including increasing slew rate, decreasing preamp frequency bandwidth, and the insertion of a lag compensation circuit in the input stage of the amplifier.[3][4][5] In high quality modern amplifiers the open loop response is at least 20 kHz, canceling TIM distortion. However, TIM distortion is still present in most low price home quality amplifiers.[citation needed]

The next step in advanced design was the Baxandall Theorem, created by Peter Baxandall in England.[6] This theorem introduced the concept of comparing the ratio between the input distortion and the output distortion of an audio amplifier. This new idea helped audio design engineers to better evaluate the distortion processes within an audio amplifier.

Applications

Important applications include public address systems, theatrical and concert sound reinforcement, and domestic sound systems. The sound card in a personal computer contains several audio amplifiers (depending on number of channels), as does every stereo or home-theatre system.

References

  1. ^ http://nobelprize.org/educational_games/physics/transistor/history/ The Transistor in a Century of Electronics
  2. ^ "Circuit Design Modifications for Minimizing Transient Intermodulation Distortion in Audio Amplifiers", Matti Otala, Journal of Audio Engineering Society, Vol 20 # 5, June 1972
  3. ^ Distribution of the Phonograph Signal Rate of Change, Lammasniemi, Jorma; Nieminen, Kari, Journal of Audio Engineering Society, Vol. 28 # 5, May 1980.
  4. ^ "Psychoacoustic Detection Threshold of Transient Intermodulation Distortion", Petri-Larmi, M.; Otala, M.; Lammasniemi, J. Journal of Audio Engineering Society, Vol 28 # 3, March 1980
  5. ^ Discussion of practical design features that can provoke or lessen slew-rate limiting and transient intermodulation in audio amplifiers can also be found for example in chapter 9 in John Linsley Hood's 'The Art of Linear Electronics' (Butterworth-Heinemann, Oxford, 1993).
  6. ^ "Audio power amplifier design", Peter Baxandall. Wireless World magazine, February 1979

See also


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Sci-Tech Encyclopedia. McGraw-Hill Encyclopedia of Science and Technology. Copyright © 2005 by The McGraw-Hill Companies, Inc. All rights reserved.  Read more
Intelligence Encyclopedia. Encyclopedia of Espionage, Intelligence, and Security. Copyright © 2004 by The Gale Group, Inc. All rights reserved.  Read more
WordNet. WordNet 1.7.1 Copyright © 2001 by Princeton University. All rights reserved.  Read more
Wikipedia. This article is licensed under the Creative Commons Attribution/Share-Alike License. It uses material from the Wikipedia article "Audio amplifier" Read more