Outline
General overview on FET
Comparison of BJT and FET
The classifications of FET
The physical structure of the JFET & MOSFET and how it works
Equations that describe VI-characteristics
FIELD-EFFECT TRANSISTORS (FETS)
How these class of transistor can be used to make an amplifier
By: Behailu T.
Field-Effect Transistors - FETs FET verses BJT
FET is a three-terminal device used for a variety of applications that Field Effect Transistor (FET) Bipolar JunctionTransistor (BJT)
match, to a large extent, those of the BJT transistor. Unipolar Bipolar
1 Current depends only on one type of Current depends on both electrons and
charge carriers holes
Both BJT and FET can be used for:
2 Voltage controlled device Current controlled device
Amplifiers 3 Very high input impedance Low input impedance
Switching devices 4
Simpler in fabrication and occupies
occupies large space in integrated form
less space in integrated form
Impedance matching circuits
Low voltage gain High voltage gain
5
High current gain Low current gain
6 Easily damaged Robust
FET: Classification JFET : Structure
Terminals: Gate - G | Drain - D | Source - S
MOSFET : Metal Oxide Semiconductor FET FET
JFET : Junction FET
MOSFET JFET
p n p
n p n
Enhancement Depletion p-channel n-channel
MOSFET MOSFET JFET JFET
n-channel JFET p-channel JFET
n-Channel p-Channel n-Channel p-Channel
EMOSFET EMOSFET DMOSFET DMOSFET
The n-channel is more widely used
JFET: Operation JFET: Operation
The JFET is always operated with the Gate-
Source pn-junction reverse-biased.
Reverse biasing of the GS-junction produces a
depletion region along the pn junction, which
extends into the n channel and thus increases
its resistance by restricting the channel width.
The channel width and thus the channel
resistance can be controlled by varying the gate
voltage, thereby controlling the amount of Physical operation of the n -channel JFET:
drain current, ID. a) For small the channel is uniform and the device functions as a resistance whose value is controlled
by (more in negative larger depletion region narrower channel lower current )
Sets the reverse-bias voltage b) Increasing causes the channel to acquire a tapered shape and eventually pinch-off occurs, so the
current reaches the max value . If = 0 the max value is
JFET: Characteristics & Parameters JFET: controls
JFET must be operated between
Pinch-Off Voltage ( ): For = 0 V, the value = 0 V and ( )
of at which becomes essentially constant
(point B on the curve).
For a given JFET, has a fixed value Active (Pinch-off) region
Drain current is (Drain to Source current
with gate Shorted) and is always specified on JFET
datasheets.
is the maximum drain current that a specific
JFET can produce regardless of the external
circuit.
Cutoff Voltage
JFET versus BJT
JFET: Transfer Characteristic
JFET transfer characteristic curve
Saturation region
is expressed approximately as :
≥−
Linear region
Active (Pinch-off) region
Saturation region
Linear region
Channel Off
Channel Off
≤− ≤−
JFET: Small-Signal Model JFET: Small-Signal Model
Transconductance: Input Impedance:
The relationship of a change in ID to Z i
the corresponding change in VGS is Output Impedance:
called transconductance 1
Z o rd
y os
Transconductance is denoted gm and
where,
given by:
VDS
ΔI D rd VGS constant
gm I D
ΔV GS
yos= admittance parameter listed on FET
specification sheets. Fig. n-channel JFET and its small signal equivalent
JFET: Common-Source(CS) Fixed-Bias Circuit JFET: Common-Source(CS) Fixed-Bias Circuit
DS
• The resistor RG is
present to ensure that
Vi appears at the input
to the FET amplifier for
the ac analysis.
• The zero-volt drop Fig. AC equivalent Circuit
across RG permits
Fig. CS Fixed-bias Circuit Fig. CS Fixed-bias Circuit
Fig. DC equivalent Circuit replacing RG by a short-
circuit equivalent.
JFET: Common-Source(CS) Fixed-Bias Circuit JFET: Common-Source(CS) Self-Bias Circuit
Input impedance:
Zi RG
Output impedance:
Z o R D || rd
Zo R D
rd 10R D
Voltage gain: Fig. AC equivalent Circuit
Vo
Av g m (rd || R D )
Vi
V
A v o g m R D Fig. CS Self-bias Circuit
Vi rd 10R D
Fig. CS Self-bias DC equivalent Circuit
JFET: Self-Bias Configuration – Graphical Soln. JFET: Common-Source(CS) Self-Bias Circuit
Fig. CS Self-bias DC
Fig. CS Self-bias Circuit Fig. CS Self-bias AC equivalent Circuit
equivalent Circuit
JFET: Common-Source(CS) Self-Bias Circuit JFET: Common-Source(CS) Voltage-divider-Bias Circuit
Input impedance:
Zi RG
Output impedance:
Z o rd || R D
Zo R D
rd 10R D
Voltage gain:
A v g m (rd || R D )
Fig. CS Voltage-divider-bias Circuit Fig. CS Voltage-divider-bias
A v g m R D Fig. CS Self-bias AC equivalent Circuit
rd 10R D DC equivalent Circuit
JFET: Common-Source(CS) Voltage-divider-Bias Circuit JFET: Common-Source(CS) Voltage-divider-Bias Circuit
Input impedance:
Z i R 1 || R 2
Output impedance:
Z o rd || R D
Zo R D
rd 10R D
Voltage gain:
A v g m (rd || R D )
Fig. CS Voltage-divider-bias AC equivalent Circuit Fig. CS Voltage-divider-bias AC equivalent Circuit
Fig. CS Voltage-divider-bias Circuit A v g m R D
rd 10R D
JFET: Reading Assignment MOSFET- Metal Oxide Semiconductor Field-Effect Transistor
Has no pn junction structure; instead,
Common-Gate Configuration the Gate of the MOSFET is insulated
from the channel by a silicon dioxide
Common-Drain(Source-Follower) Configuration
(SiO2) layer.
The two basic types of MOSFETs
are:
Enhancement(E) MOSFET &
Depletion(D) MOSFET
The enhancement MOSFET is more Symbols for: (a) n-channel symbols for: (a) n-channel
enhancement-type depletion-type MOSFETs
widely used. and (b) p-channel depletion-
MOSFETs and (b) p-channel
enhancement type type MOSFETs.
MOSFETs.
Depletion-Type MOSFET Construction D-MOSFET: Operation and Characteristics
The Drain (D) and Source (S) connect to
the n-doped regions. = 0 and is applied across the drain-
These n-doped regions are connected via an source terminals
n-channel. This results to attraction of free electrons of
This n-channel is connected to the Gate(G)
the n-channel to the drain, and hence
via a thin insulating layer of SiO2.
current flows.
The n-doped material lies on a p-doped
substrate that may have an additional
terminal connection called Substrate(SS).
Fig. n-Channel depletion-type MOSFET
with VGS = 0 V and applied voltage VDD.
D-MOSFET: Operation and Characteristics D-MOSFET: Operation and Characteristics
For negative value of , the negative potential at For positive values of , the positive gate will A depletion-type MOSFET can
operate in two modes:
the gate pressures electrons toward the p-type draw additional electrons (free carriers) from the
p-type substrate and hence increases. Depletion Mode
substrate and attract holes from p-type substrate.
The characteristics are similar to a
This will reduce the number of free electrons in JFET.
When =0 , =
the n-channel available for conduction. When <0 , <
The more negative the , the resulting level of Enhancement Mode
drain current is reduced. >0
increases above
When is reduced to (Pinchoff voltage), then
= 0mA. The formula used to plot the transfer
curve still applies:
Fig. Reduction in free carriers in a channel
due to a negative potential at the gate
= −
terminal.
p-channel D-Type MOSFET Enhancement-Type MOSFET Construction
The Drain(D) and Source(S) connect
to the n-doped regions.
The Gate(G) connects to the p-doped
substrate via a thin insulating layer of
SiO2.
There is no physical channel.
The n-doped material lies in the p-
doped substrate that may have an
additional terminal connection called
the Substrate (SS).
Fig. n-channel enhancement-type MOSFET.
E-MOSFET : Operation and Characteristics E-MOSFET : Operation and Characteristics
For = 0 , = 0 (no channel). The enhancement-type MOSFET operates
For some positive voltage, and = 0, two only in the enhancement mode.
reverse biased pn-junctions and no significant
is always positive.
flow between Drain and Source.
For > 0 and > 0 , the positive voltage
As increases, increases.
at Gate pressure holes to enter deeper regions As is kept constant and is increased,
of the p-substrate, and the electrons in the p- then saturates and the saturation level,
substrate will be attracted to the positive Gate. is reached.
The level of that results in the significant = -
increase in the Drain current is called threshold
voltage ( ).
For < , = 0mA.
Fig. For the case of > 0 and >0
E-MOSFET : Operation and Characteristics
MOSFET: Reading Assignment
MOSFET Small Signal Model Analysis