SEC. 13-1 BASIC IDEAS
The junction FET, abbreviated JFET, has a
source, gate, and drain. The JFET has two
diodes: the gate-source diode and the
gate-drain diode. For normal operation,
the gate-source diode is reverse biased.
Then, the gate voltage controls the drain
current.
SEC. 13-2 DRAIN CURVES
Maximum drain current occurs when the
gate-source voltage is zero. The pinchoff
voltage separates the ohmic and active
regions for VGS = 0. The gate-source
cutoff voltage has the same magnitude
as the pinchoff voltage. VGS(off) turns the
JFET off.
SEC. 13-3 THE TRANSCONDUCTANCE
CURVE
This is a graph of drain current versus
gate-source voltage. The drain current
increases more rapidly as VGS approaches
zero. Because the equation for drain
current contains a squared quantity,
JFETs are referred to as square-law
devices. The normalized transconductance
curve shows that ID equals
one-quarter of maximum when VGS
equals half of cutoff.
SEC. 13-4 BIASING IN THE
OHMIC REGION
Gate bias is used to bias a JFET in the
ohmic region. When it operates in the
ohmic region, a JFET is equivalent to a
small resistance of RDS. To ensure
operation in the ohmic region, the JFET
is driven into hard saturation by using
VGS = 0 and ID(sat) « IDSS.
SEC. 13-5 BIASING IN THE
ACTIVE REGION
When the gate voltage is much larger than
VGS, voltage-divider bias can set up a stable
Q point in the active region. When positive
and negative supply voltages are available,
two-supply source bias can be used to
swamp out the variations in VGS and set up
a stable Q point. When supply voltages are
not large, current-source bias can be used
to get a stable Q point. Self-bias is used
only with small-signal amplifiers because
the Q point is less stable than with the
other biasing methods.
SEC. 13-6 TRANSCONDUCTANCE
Transconductance gm tells us how
effective the gate voltage is in controlling
the drain current. The quantity gm is the
slope of the transconductance curve,
which increases as VGS approaches zero.
Data sheets may list gfs and siemens,
which are equivalent to gm and mhos.
SEC. 13-7 JFET AMPLIFIERS
A CS amplifier has a voltage gain of gmrd
and produces an inverted output signal.
One of the most important uses of a JFET
amplifier is the source follower, which is
often used at the front end of systems
because of its high input resistance.
SEC. 13-8 THE JFET ANALOG
SWITCH
In this application, the JFET acts like a
switch that either transmits or blocks
a small ac signal. To get this type of
action, the JFET is biased into hard
saturation or cutoff, depending on
whether VGSis high or low. JFET shunt
and series switches are used. The series
type has a higher on-off ratio.
SEC. 13-9 OTHER JFET
APPLICATIONS
JFETs are used in multiplexers (ohmic),
chopper amplifiers (ohmic), buffer
amplifiers (active), voltage-controlled
resistors (ohmic), AGC circuits (ohmic),
cascode amplifiers (active), current
sources (active), and current limiters
(ohmic and active).
SEC. 13-10 READING DATA
SHEETS
JFETs are mainly small-signal devices
because most JFETs have a power rating
of less than 1 W. When reading data
sheets, start with the maximum ratings.
Sometimes data sheets omit the
minimum VGS(off ) or other parameters.
The large spread in JFET parameters
justifies using ideal approximations for
preliminary analysis and troubleshooting.
SEC. 13-11 JFET TESTING
JFETs can be tested using an ohmmeter or
DMM on the diode test range. Care must
be taken not to exceed the JFET’s current
limits. Curve tracers and circuits can be
used to display a JFET’s dynamic
characteristics.
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