Electronics Circuits 1 JFET amplifier and biasing

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Andrzej Materka
Electronics Circuits 1
JFET amplifier and biasing
Telecommunications and Computer Science
90-924 Łódź, ul. Wólczańska 211/215
tel. 42 631 2626, 42 636 0065
www.eletel.p.lodz.pl
n-channel, junction
field-effect transistor (FET)
Drain
D
Channel
Gate
p
n
p
G
S
Source
Physical structure
Circuit symbol
A. Materka, Electronics Circuits 1, JFET Amplifier and Biasing
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n-channel, junction FET
iD (mA)
iD
Linear
region
D
G
+
vGS
vDS
Saturation
region
vGS=0
10
+
vGS=-1V
5
S
vGS=-2V
Circuit for discussion
of DC characteristics
0
0
5
10
vDS (V)
Cutoff vGS<VP
Drain DC characteristics of an n-channel JFET
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n-channel, junction FET
Cut-off region
iD (mA)
iD  0, vGS  VP
Linear
region
Saturation
region
vGS=0
10
Linear region

2
i D  K 2vGS  VP v DS  v DS
vGS  VP and
vGD  (vGS  v DS )  VP

vGS=-1V
5
vGS=-2V
iD
0
0
5
10
vDS (V)
Cutoff vGS<VP
Saturation region
Spice model parameters
I DSS
2
iD  2 vGS  VP  ,
VP
I DSS
2 =„Beta”, Vp=„Vto”
VP
vGS
VP
vGS  V P and
Transfer characteristic
vGD  (vGS  v DS )  V P
in saturation
Typical for low-power JFET:
IDSS=5mA, VP=-3V
A. Materka, Electronics Circuits 1, JFET Amplifier and Biasing
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Simple JFET amplifier
iD
RD
1k
D
G
+
vin(t)
iD (mA)
+ 20V
vDS
VDD
Load
line
20
A
sin(2000t)
VGG
vGS
vGS=0
S
+
Q-point
10
vGS=-1V
1V
vGS (t )  vin (t )  VGG
B
vGS (t )  sin(2000t )  1
VDD  RDi D (t )  v DS (t )
20  iD (t )[mA]  vDS (t )
0
0
10
VDSmin=4V
vGS=-2V
20
vDS (V)
VDS=11V VDSmax=16V
The output waveform is not a symmetrical
sinusoid like the input (nonlinear distortion).
A. Materka, Electronics Circuits 1, JFET Amplifier and Biasing
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Simple JFET amplifier , VG =-1V
Model tranzystora FET
.model JF NJF(Beta=1m Vto=-4V)
VD
VG
Voltage gain is rather modest (Av ≈ -6),
current gain tends to infinity.
A. Materka, Electronics Circuits 1, JFET Amplifier and Biasing
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Simple JFET amplifier, VG =-2V
Model tranzystora FET
.model JF NJF(Beta=1m Vto=-4V)
VD
VG
Av ≈ -4
A. Materka, Electronics Circuits 1, JFET Amplifier and Biasing
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Simple JFET amplifier, VG =-2V
Model tranzystora FET
.model JF NJF(Beta=1m Vto=-4V)
VD
VG
Av ≈ -2
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iD
RD
D
G
+
vin(t)
JFET amplifier
1k
vDS
+ 20V
VDD
sin(2000t)
VGG
vGS
S
+
1V
Both the gain and distortion depend on bias
(on selection of Q-point – quiescent point of
transistor operation).
A. Materka, Electronics Circuits 1, JFET Amplifier and Biasing
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iD
RD
D
G
+
vin(t)
vGS
+
+ 20V
vDS
sin(2000t)
VGG
JFET amplifier
1k
S
VDD
Both the gain and distortion depend on bias
(on selection of Q-point – quiescent point of
transistor operation).
1V
Analysis of amplifiers is done in two steps:
- determination of the Q-point
(using a nonlinear device model),
- finding the input resistance, voltage gain, etc.
(linear ac analysis using a small-signal
equivalent circuit).
A. Materka, Electronics Circuits 1, JFET Amplifier and Biasing
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iD
RD
D
G
+
vin(t)
vDS
sin(2000t)
VGG
vGS
+
JFET dc bias
1k
S
+ 20V
VDD
Two-battery bias circuit is not practical
(usually one battery is available only).
iD
1V
Values of JFET parameters vary
considerably from device to device,
e.g. IDSS may vary by a ratio of 5:1,
the pinch-off voltage is different from
device to device.
ID
ID
Fixed-bias circuit (maintaining a constant VGS) is not suitable.
It would lead to a considerable variation of ID. The Q-point would be
located far from the middle of the load line, causing considerable
output waveform distortion and a loss of gain from device to device.
vGS
VGS
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iD
JFET self-bias circuit
RD
D
G
vGS
RG
RS
+
vDS
VDD
iD
Neglecting the gate current one has
S
vGS   RS i D
RSiD
Bias line
vGS=-RSiD
Graphical analysis of the self-bias circuit
The device-to-device variation of drain current is
much less than for the fixed-bias circuit.
vGS
VGS VGS
VDD is of such a value that VDS is large enough
for operation in the saturation region.
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JFET self-bias circuit
iD
RD
D
G
vGS
RG
RS
+
vDS
S
RSiD
VDD
Exercise 4.1 Design a self-bias circuit for an n-channel
FET having IDSS =4mA and VP =-2V. The circuit is to have
RD =2.2k, VDD =20V, and ID 2mA. Use standard 10%tolerance resistor values. Answer: RS=270.
Exercise 4.2 Analyse the self-bias circuit designed in Exercise 4.1.
Repeat the analysis for a high-current device having IDSS=8mA and
VP=-4V. Verify your results with SPICE.
Answer:
VGS=-0.56V, ID=2.07mA, VDS=14.9V;
VGS=-1.12V, ID=4.14mA, VDS=9.77V.
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iD
The Fixed- Plus Self-Bias Circuit
RD
D
R1
G
VDD
vDS
vGS
R2
+
Gives better performance in maintaining
a fixed ID from device to device.
S
RS
RSiD
- The Thevenin voltage: VG  VDD
iD
- The Thevenin resistance: RG = R1 || R2
RD
D
RG
G
vGS
VG
RS
R2
R1  R2
+
vDS
S
RSiD
VG=0 corresponds
to self-bias.
VDD
- Voltage equation: VG  vGS  RS i D (VRG  0)
(4.17)
2
- Assumed saturation: i D  KvGS  V P 
(4.18)
- Simultaneous solution of (4.17) and (4.18) yields the
operating point.
- v DS  VDD  ( RD  RS )is
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The Fixed- Plus Self-Bias Circuit
iD
RD
D
RG
G
vGS
VG
RS
iD
+
vDS
VDD
S
RSiD
Equation (4.17)
vGS
VG
Graphical solution for the fixed- plus self-bias circuit;
ID is nearly independent of the device if VG is large.
In practice, VG can not be too high because this raises the
voltage drop across RS, and sufficient voltage must be
allocated for vDS and RD.
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The Fixed- Plus Self-Bias Circuit
iD
RD
D
RG
G
vGS
VG
RS
+
vDS
S
RSiD
VDD
Exercise 4.3 Design for VG5V a fixed- plus self-bias
circuit for the JFET of Exercise 4.1 having IDSS=4mA and
VP=-2V. The circuit is to have RD=2.2k, VDD=20V, and
ID2mA. Use standard 10%-tolerance resistor values.
Answer: RS=2.7k.
Exercise 4.4 Analyse the self-bias circuit designed in Exercise 4.3.
Repeat the analysis for a high-current device having IDSS=8mA and
VP=-4V. Verify your results with SPICE.
Answer:
VGS=-0.564V, ID=2.06mA, VDS=9.9V;
VGS=-1.76V, ID=2.50mA, VDS=7.73V.
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