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Chapter 2 Small-Signal Amplifiers

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Chapter 2 Small-Signal Amplifiers Most amplifiers in communication circuits are small signal amplifiers. Hence, they can be described by linear equations. – PowerPoint PPT presentation

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Title: Chapter 2 Small-Signal Amplifiers


1
Chapter 2Small-Signal Amplifiers
  • Most amplifiers in communication circuits are
    small signal amplifiers. Hence, they can be
    described by linear equations. We will consider
    several amplifiers including BJT, FET,
    operational amplifiers and differential
    amplifiers.

Bipolar Transistor Amplifiers
  • The equivalent circuit of the BJT is shown below

2
  • rb is the resistance between the terminal and
    the actual base junction, r? is the base-emitter
    junction resistance.
  • Typically r? gtgt rb. An estimation of r? is
  • r0 is the collector to emitter resistance
    typically of the order 15k?, r? is the
    collector-base resistance of the order several
    M?.
  • The transconductance gm r? ?
  • A simplified version of the small-signal model
    equivalent circuit is given below

3
Common-Emitter Amplifier
  • here the coupling capacitance is treated as a
    short circuit.
  • The output voltage is therefore
  • The input impedance, not including Rs, is given
    be
  • Since r? depends on applied the input resistance
    will depend on it as well.
  • The current gain is

4
Common Base Amplifier
  • The Circuit diagram and its equivalent circuit
    model for the CB amplifier are shown below
  • Since the sum of the currents leaving the emitter
    junction is 0, we have the following expression

5
  • If r0 is assumed to be large compared with Rs, r?
    and RL, the voltage gain is
  • if r? gtgt Rs(1?), the magnitude of the voltage
    gain will be the same as that of the
    common-emitter amplifier
  • The input impedance of the common-base amplifier
    is determined using the following circuit

6
  • The output impedance is determined using the
    following circuit
  • The common-base amplifier has a voltage gain but
    its current gain is less than unity. It is used
    as non-inverting amplifiers where low input
    impedance and high output impedance is desired.
  • It also has much better high-frequency response
    than CE amplifier and is often used in
    high-frequency circuits.

7
Emitter Follower
  • The EF has a non-inverting voltage gain of less
    than 1
  • However, it can combine with other stages, such
    as the CE stage, to realize a greater combined
    gain than CE stage alone

8
  • Using the equivalent circuit the voltage gain if
    found to be
  • EF configuration has the largest input impedance
    compared to the other configurations

9
  • The output impedance is
  • EF is used when low output impedance is needed.
    Also, although it has a voltage gain lt 1, it has
    large current gain. It is frequently used as a
    power amplifier for low-impedance loads.

10
Field-Effect Transistors Amplifiers
  • There are two types of FETs -- JFETs and MOSFETs.
  • The low-frequency small signal model is as shown
  • The transconductance is defined as
  • For JFETs
  • where gm0 is the transconductance when
    gate-to-source bias voltage is 0, ID is the drain
    current and IDSS is the drain current when the
    gate-to-source voltage is 0.
  • For MOSFETs, gm is
  • where gmR is the transconductance at some
    specified drain bias current IDR

11
Common-Source Amplifier
  • The common-source amplifier is similar to the
    common-emitter amplifier
  • The common-source amplifier is similar to the
    common-emitter amplifier.
  • Normally Rg gtgt R so Vi Vg

12
  • The source voltage is determined from the
    following equations
  • since the current leaving output node and source
    is zero
  • The current through Rs The source voltage is
  • The voltage gain is
  • If rd gtgt Rs and RL we have the following
    relationship
  • For gm Rs gtgt 1 we have

13
Source-Follower
  • The circuit diagram and its equivalent circuit
    model for source follower are shown below
  • If Rb gtgt Rs, then

14
Common-Gate Amplifier
  • The output impedance is
  • which is much smaller than the other two FET
    amplifier configurations and is the major
    advantage for this configuration
  • The common-gate amplifier is often used in
    high-frequency application and has a much larger
    bandwidth than the common source configuration.

15
  • Thus
  • The input impedance at the source can be found by
    solving for the source current
  • and
  • since

16
Multistage Amplifiers
  • The output impedance is determined as
  • but I0 is also the current passing through the
    source resistance so
  • The common gate amplifier has the highest output
    impedance of the three FET amplifier
  • Multistage amplifiers are used for impedance
    matching or to obtain extra gain.
  • Power transistors have smaller gain-bandwidth
    product than low-power transistors, hence the
    power amplification stage is often operated near
    unity voltage gain in order to maximize the
    bandwidth
  • Voltage amplification is carried out in the
    stages preceding the power amplification stage

17
Dual Gate FET
  • The FET cascode circuit has many high-frequency
    applications that two FETs are often fabricated
    as a single transistor with 2 gates. The source
    of the one transistor is continuous with the
    drain of the other so the device has 1 source, 1
    drain and 2 gates
  • The device offers low-noise and high gain in
    radio-frequency applications
  • It is a versatile device which can be used as a
    mixer or automatic gain control amplifier. The
    equivalent circuit is as shown

18
  • Here gate 2 and the source are grounded
  • The load resistance of the first stage is the
    input resistance of the second stage, and the
    second stage is a common-gate amplifier.
    Therefore
  • Since
  • where gmR is the transconductance at some
    specified drain bias current IDR.
  • Since both transistors have the same drain
    current gm1gm2. Thus Vi-VD1 and Vgs2-Vs2-VD1

19
Push Pull Amplifiers
  • Transistors all exhibit a nonlinear
    characteristic that causes distortion of the
    input signal levels. Such distortion can be
    eliminated by push-pull amplifier
  • The above example uses 2 center-tapped
    transformers. The input transformer separates
    the input signal into 2 signal 180? out of phase.
    The output transformer is used to sum the output
    currents of the two transistors.
  • Hence
  • If the input signal is

20
  • then the output of the 2 transistors are also
    periodic, and they can be expressed in a Fourier
    series
  • If the two transistors are identical then I1 and
    I2 are identical except I2 lags I1 by 180 ?.
    Thus
  • The output current is
  • The even harmonics are eliminated from the
    output. This is important as FET have a
    square-law characteristic that generates a
    relatively large second harmonic.

21
Differential Amplifier
  • The differential amplifier is an essential
    building block in modern IC amplifiers. The
    circuit is shown below
  • The operation of this circuit is based on the
    ability to fabricate matched components on the
    same chip. In the figure IEE is realized using a
    current mirror. We assume that Q1 and Q2 are
    identical transistors and both collector
    resistors fabricated with equal values.
  • The KVL expression for the loop containing the
    two emitter-base junctions is

22
  • The transistors are biased in the forward-active
    mode, the reverse saturation current of the
    collector-base junction is negligible. The
    collector currents IC1 and IC2 are given by
  • where we assumed that
  • where Vd is the difference between the two input
    voltages. KCL at the emitter node requires
  • Similarly The
    transfer
  • characteristic for the emitter-coupled pair is
    shown on the following page.
  • If Vd 0 then IC1 IC2

23
  • If we incrementally increase V1 by
    and simultaneously decrease V2 by .
    The differential voltage becomes . For
    lt 4kT as indicated in the transfer
    characteristics above the circuit behaves
    linearly. IC1 increases by and IC2
    decreases by the same amount.

24
Common Mode
  • Consider both V1 and V2 are increased by
    . The difference voltage remains 0, and IC1
    and Ic2 remain equal. However, both IC1 and Ic2
    exhibit a small increase . Hence the
    current in RE increases by . The
    voltage VE is no longer constant but increase by
    an amount of . This situation
    where equal signal are applied to Q1 and Q2 is
    the called the common mode.
  • Usually differential amplifiers are designed such
    that only differential signals are amplified.

Analysis of Differential Amplifiers
  • The analysis of differential amplifiers is
    simplified using half-circuit concept. The
    equivalent circuit model for differential and
    common modes are shown

25
  • Differential mode gain
  • Common mode gain is
  • The Common Mode Rejection Ration (CMRR) is
    defined as
  • From the above we obtain
  • If arbitrary signals V1 and V2 are applied to the
    inputs then

26
FET Differential Amplifier
  • A typical differential amplifier connection is
    shown below
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