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FET amplifier
FET amplifier
from Wikipedia
Generalised FET as an amplifier

An FET amplifier is an amplifier that uses one or more field-effect transistors (FETs). The most common type of FET amplifier is the MOSFET amplifier, which uses metal–oxide–semiconductor FETs (MOSFETs). The main advantage of a FET used for amplification is that it has very high input impedance and low output impedance.

In detail

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The transconductance is given by

On rearranging, we get

Equivalent circuit

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The internal resistance Rgs, between gate and source appears between drain and source. Rds is the internal resistance between the drain and source. As Rgs is very high, it is taken to be infinite, and Rds is neglected. [1]

Voltage gain

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For ideal FET equivalent circuit, voltage gain is given by,

From the equivalent circuit,

and from the definition of transconductance,

we get[1]

Types of FET amplifiers

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There are three types of FET amplifiers, depending on which terminal is the common input and output. (This is similar to a bipolar junction transistor (BJT) amplifier.)

Common gate amplifier

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The gate is common to both input and output.

Common source amplifier

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The source is common to both input and output.

Common drain amplifier

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The drain is common to both input and output. It is also known as a "source follower".[2]

History

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The basic principle of the field-effect transistor (FET) amplifier was first proposed by Austro-Hungarian physicist Julius Edgar Lilienfeld in 1925.[3] However, his early FET concept was not a practical design.[4] The FET concept was later also theorized by Oskar Heil in the 1930s and William Shockley in the 1940s,[5] but there was no working practical FET built at the time.[4]

MOSFET amplifier

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A breakthrough came with the work of Egyptian engineer Mohamed M. Atalla in the late 1950s.[6] He developed the method of surface passivation, which later became critical to the semiconductor industry as it made possible the mass-production of silicon semiconductor technology, such as integrated circuit (IC) chips.[7][4][8] For the surface passivation process, he developed the method of thermal oxidation, which was a breakthrough in silicon semiconductor technology.[9] The surface passivation method was presented by Atalla in 1957.[10] Building on the surface passivation method, Atalla developed the metal–oxide–semiconductor (MOS) process,[7] with the use of thermally oxidized silicon.[11][12] He proposed that the MOS process could be used to build the first working silicon FET, which he began working on building with the help of Korean recruit Dawon Kahng.[7]

The MOS field-effect transistor (MOSFET) amplifier was invented by Mohamed Atalla and Dawon Kahng in 1959.[5] They fabricated the device in November 1959,[13] and presented it as the "silicon–silicon dioxide field induced surface device" in early 1960,[14] at the Solid-State Device Conference held at Carnegie Mellon University.[15] The device is covered by two now long-expired patents, each filed separately by Atalla and Kahng in March 1960.[16][17]

See also

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References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
A field-effect transistor (FET) amplifier is an electronic circuit that uses one or more field-effect transistors to amplify the amplitude of an input electrical signal while preserving its waveform. FETs, such as junction field-effect transistors (JFETs) and metal-oxide-semiconductor field-effect transistors (MOSFETs), operate as voltage-controlled devices where a gate voltage modulates the conductivity between the drain and source terminals, enabling linear amplification in the saturation region. The basic principle of FET amplification relies on the parameter gmg_m, which relates changes in output drain current to variations in input gate-source voltage, typically analyzed using small-signal models for AC signals superimposed on a point. JFETs are depletion-mode devices that conduct current at zero gate and require a reverse to reduce channel conductivity up to a pinch-off voltage, while MOSFETs are enhancement-mode devices that require a positive gate voltage to form a conductive channel. This field-effect control results in extremely high at the , often in the gigaohm range or higher, minimizing loading effects on preceding circuit stages. FET amplifiers are configured in three primary topologies: the common-source arrangement, which provides high voltage gain (often inverting and greater than 1 in magnitude) suitable for general amplification; the common-drain (or source-follower), which offers unity gain with low output impedance for buffering applications; and the common-gate, which delivers unity current gain with low input impedance for . Key performance metrics include voltage gain Av=gmRDA_v = -g_m R_D for common-source stages, where RDR_D is the drain resistance, and overall characteristics like moderate output resistance and low . Compared to (BJT) amplifiers, FET amplifiers excel in applications requiring minimal power dissipation, compact integration in ICs, and low-noise performance due to their voltage-driven nature and absence of base current. They are widely used in audio preamplifiers, RF front-ends, and sensor interfaces where high is critical.

Fundamentals

Basic Principles

A (FET) is a three-terminal that operates as a voltage-controlled , where the voltage applied to the terminal modulates the conductivity of a channel between the source and drain terminals, thereby controlling the drain-source current (IDI_D). This field-effect relies on the generated by the gate voltage to influence the density of charge carriers in the channel without requiring gate current, distinguishing it from current-controlled devices. FETs function in two primary modes: depletion mode and enhancement mode. In depletion-mode operation, the channel is inherently conductive at zero gate-to-source voltage (VGS=0V_{GS} = 0), and applying a reverse to the gate depletes the channel of carriers, reducing IDI_D; this mode is common in junction FETs (JFETs). Conversely, enhancement-mode FETs, prevalent in metal-oxide-semiconductor FETs (MOSFETs), have a non-conductive channel at VGS=0V_{GS} = 0, requiring a forward gate to induce carriers and form the channel, thereby increasing IDI_D. These modes enable versatile biasing for amplification tasks. In amplification, the FET exploits its voltage sensitivity such that a small input signal applied to the produces a proportionally larger variation in the drain current, which can drive a load to yield an amplified output voltage. The primary for this gain mechanism is the (gmg_m), defined as the of drain current with respect to gate-source voltage at constant drain-source voltage: gm=IDVGSVDS=\constantg_m = \left. \frac{\partial I_D}{\partial V_{GS}} \right|_{V_{DS} = \constant}
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