Transcript Bates
Chapter
30
Field Effect Transistors
Topics Covered in Chapter 30
30-1: JFETs and Their Characteristics
30-2: Biasing Techniques for JFETs
30-3: JFET Amplifiers
30-4: MOSFETs and Their Characteristics
30-5: MOSFET Biasing Techniques
30-6: Handling MOSFETs
© 2007 The McGraw-Hill Companies, Inc. All rights reserved.
30-1: JFETs and Their Characteristics
Fig. 30-1 (a) in the next slide, shows the construction
of an n-channel JFET.
There are four leads: the drain, source, and two gates.
The area between the source and drain terminals is
called the channel.
Because n-type semiconductor material is used for the
channel, the device is called an n-channel JFET.
Embedded on each side of the n-channel are two
smaller p-type regions called gates.
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© 2007 The McGraw-Hill Companies, Inc. All rights reserved.
30-1: JFETs and Their Characteristics
JFET
P-Channel
N-Channel
Fig. 30-1
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30-1: JFETs and Their Characteristics
Fig. 30-2 (a) is the schematic symbol for the n-channel JFET, and Fig. 30-2 (b)
shows the symbol for the p-channel JFET.
The only difference is the direction of the arrow on the gate lead.
Fig. 30-2 (a)
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Fig. 30-2 (b)
30-1: JFETs and Their Characteristics
Fig. 30-3 illustrates the current
flow in an n-channel JFET with ptype gates disconnected.
The amount of current depends
upon two factors:
The value of the drainsource voltage, VDS
The drain-source
resistance, designated rDS
Fig. 30-3
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30-1: JFETs and Their Characteristics
The gate regions in a JFET are embedded on each side of the channel
to help control the amount of current flow in the channel.
Fig. 30-4 (a) shows an n-channel JFET with both gates shorted to the
source.
Fig. 30-4 (b) shows how an n-channel JFET is normally biased.
Fig. 30-4
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30-1: JFETs and Their Characteristics
Fig. 30-5 (a) shows an n-channel JFET connected to the proper biasing
voltages.
The drain is positive and the gate is negative, creating the depletion
layers.
Fig. 30-5 (c) shows a complete set of drain curves for the JFET in Fig.
30-5 (a).
Fig. 30-5 (a) (c)
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30-2: Biasing Techniques for JFETs
Many techniques can be used to bias JFETs.
In all cases, the gate-source junction is reverse-
biased.
The most common biasing techniques are
Gate
Self
Voltage-divider
Current-source
30-2: Biasing Techniques for JFETs
Fig. 30-7 (a) shows an example of gate bias.
Fig. 30-7 (b) shows how an ac signal is coupled to the gate of a JFET.
If RG were omitted, as shown in (c), no ac signal would appear at the
gate because VGG is at ground for ac signals.
Fig. 30-7
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30-2: Biasing Techniques for JFETs
One of the most common ways to bias a JFET is with self-bias. (See Fig.
30-8 a)
Only a single power supply is used, the drain supply voltage, VDD.
Fig. 30-8
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30-2: Biasing Techniques for JFETs
Fig. 30-9 shows a JFET with
voltage-divider bias.
Since the gate-source junction
has extremely high resistance, the
R1 – R2 voltage divider is
practically unloaded.
Voltage-divider bias is more
stable than either gate or self-bias.
Fig. 30-9
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30-2: Biasing Techniques for JFETs
Fig. 30-10 shows one of the best
ways to bias JFETs, called currentsource bias.
The npn transistor with emitter bias
acts like a current source for the JFET.
The drain current , ID, equals the
collector current, IC, which is
independent of the value of VGS.
Fig. 30-10
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30-3: JFET Amplifiers
JFETs are commonly used to amplify small ac signals.
One reason for using a JFET instead of a bipolar
transistor is that very high input impedance, Zin, can
be obtained.
A big disadvantage, however, is that the voltage gain,
AV, obtainable with a JFET is much smaller.
JFET amplifier configurations are as follows:
Common-source (CS)
Common-gate (CG)
Common-drain (CD)
30-3: JFET Amplifiers
Fig. 30-12 (a) shows a common-source amplifier.
For a common-source amplifier, the input voltage is applied to the gate
and the output is taken at the drain.
Fig. 30-12 (a)
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30-3: JFET Amplifiers
The ac equivalent circuit is shown in Fig. 30-12 (b)
On the input side, RG = Zin, which is 1 MΩ.
This occurs because with practically zero gate current, the gate-source
resistance, designated RGS, approaches infinity.
Fig. 30-12 (b)
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30-3: JFET Amplifiers
Fig. 30-13 (a) shows a common-drain amplifier, usually referred to as a
source follower.
A source follower has a high input impedance, low output impedance,
and a voltage gain of less than one, or unity.
Fig. 30-13 (a)
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30-3: JFET Amplifiers
A common-gate amplifier has a moderate voltage gain.
Its big drawback is that Zin is quite low.
Fig. 30-14 (a) shows a CG amplifier.
Fig. 30-14 (a)
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30-4: MOSFETs and Their
Characteristics
The metal-oxide semiconductor field effect
transistor has a gate, source, and drain just like the
JFET.
The drain current in a MOSFET is controlled by the
gate-source voltage VGS.
There are two basic types of MOSFETS: the
enhancement-type and the depletion-type.
The enhancement-type MOSFET is usually referred to
as an E-MOSFET, and the depletion-type, a DMOSFET.
The MOSFET is also referred to as an IGFET because
the gate is insulated from the channel.
30-4: MOSFETs and Their
Characteristics
Fig. 30-15 (a) shows the construction of an n-channel depletion-type
MOSFET, and Fig. 30-15 (b) shows the schematic symbol.
Fig. 30-15
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30-4: MOSFETs and Their
Characteristics
Fig. 30-19 shows the construction and schematic symbol for a p-
channel, depletion-type MOSFET.
Fig. 30-19 (a) shows that the channel is made of p-type semiconductor
material and the substrate is made of n-type semiconductor material.
Fig. 30-19 (b) shows the schematic symbol.
Fig. 30-19
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30-4: MOSFETs and Their
Characteristics
Fig. 30-20 (a) shows the
construction of an n-channel,
enhancement-type MOSFET.
The p-type substrate makes
contact with the SiO2 insulator.
Because of this, there is no
channel for conduction
between the drain and source
terminals.
Fig. 30-20 (a)
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30-5: MOSFET Biasing Techniques
Zero-bias can be used only with depletion-type
MOSFETs.
Even though zero bias is the most commonly used
technique for biasing depletion-type MOSFETs, other
techniques can also be used.
Biasing techniques include
Self
Voltage-divider
Current-source
Drain-feedback bias is often used to bias E-MOSFETs
30-5: MOSFET Biasing Techniques
Fig. 30-22 (a) shows a popular biasing technique that can be used only
with depletion-type MOSFETs.
This form of bias is called zero bias because the potential difference
between the gate-source region is zero.
Fig. 30-22 (a)
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30-6: Handling MOSFETs
One disadvantage of MOSFET devices is their
extreme sensitivity to electrostatic discharge (ESD)
due to their insulated gate-source regions.
The SiO2 insulating layer is extremely thin and can be
easily punctured by an electrostatic discharge.
The following is a list of MOSFET handling
precautions
Never insert or remove MOSFETs from a circuit with the
power on.
30-6: Handling MOSFETs
MOSFET handling precautions (Continued)
Never apply input signals when the dc power supply is
off.
Wear a grounding strap on your wrist when handling
MOSFET devices.
When storing MOSFETs, keep the device leads in
contact with conductive foam, or connect a shorting ring
around the leads.