8.4 FET AMPLIFIERS 407
Rin=R 1 ‖R 2 =
300 ( 100 )
400
=75 k
Ai=
Rin
RL
Av 1 =
75
3
(− 2 )=− 50
Common-Drain (CD) JFET Amplifier
Figure 8.4.2(a) shows a CD JFET amplifier in which resistorsR 1 ,R 2 , andRSSare selected by the
bias design, and capacitorsCGandCSare chosen to be large enough to act as short circuits at
frequencies in the band of interest (known as the midband). Figure 8.4.2(b) gives its small-signal
ac equivalent circuit. Analysis of this circuit yields
Ri∼=∞ (8.4.6)
Rin=R 1 ‖R 2 =
R 1 R 2
R 1 +R 2
(8.4.7)
Av 1 =
vL
v 1
=
gmro(RSS‖RL)
ro+(RSS‖RL)( 1 +gmro)
(8.4.8)
Ai=
iL
iS
=
gmro(RSS‖RL)(R 1 ‖R 2 )
RL[ro+(RSS‖RL)( 1 +gmro)]
(8.4.9)
In many casesAv 1 ∼=1 andvL=v 1 ; that is to say the load voltage “follows” the input. Hence a
CD amplifier is often known as asource follower, which becomes an excellent buffer to couple a
high-resistance source to a low-resistance load with nearly no loss in signal voltage. The current
gain, however, can be very large, leading to significant power gain.
Common-Gate (CG) JFET Amplifier
Figure 8.4.3(a) shows a CG JFET amplifier in which resistorsR 1 ,R 2 ,RD,andRSSare selected by
the bias design, and capacitorsCDandCSare chosen to be large enough to act as short circuits at
R 1
R 2
(a)
RS
+
−
vS
Input ac source
CG
Output
voltage
Rin
+
−
VDD
Ri
RSS
G
S
D
+
−
vL
CS
Ground
RL
n- Channel
JFET
Figure 8.4.2Common-drain (CD) JFET amplifier.(a)Circuit.(b)Small-signal ac equivalent circuit.