
Chapter 3 The Field-Effect Transistor 155
Rearranging this equation produces
K
n
R
D
(V
GS
− V
TN
)
2
+(V
GS
− V
TN
) − V
DD
= 0
or
(0.1)(20)(V
GS
− V
TN
)
2
+(V
GS
− V
TN
) − 5 = 0
Solving the quadratic equation, we find that
V
GS
− V
TN
= 1.35 V = V
DS
Therefore,
V
GS
= 2.35 V
and
I
D
= (0.1)(2.35 −1)
2
= 0.182 mA
Comment: For
V
GS
< 2.35 V
, the transistor is biased in the saturation region; for
V
GS
> 2.35 V
, the transistor is biased in the nonsaturation region.
EXERCISE PROBLEM
Ex 3.7: Consider the circuit in Figure 3.30. Using the nominal transistor parame-
ters described in Exercise Ex 3.6, draw the load line and determine the transition
point parameters. (Ans.
V
SG
= 2.272 V, I
D
= 0.4668 mA, V
SD
= 1.972 V)
Problem-Solving Technique: MOSFET DC Analysis
Analyzing the dc response of a MOSFET circuit requires knowing the bias con-
dition (saturation or nonsaturation) of the transistor. In some cases, the bias
condition may not be obvious, which means that we have to guess the bias condi-
tion, then analyze the circuit to determine if we have a solution consistent with our
initial guess. To do this, we can:
1. Assume that the transistor is biased in the saturation region, in which case
V
GS
> V
TN
,
I
D
> 0
, and
V
DS
≥ V
DS
(sat)
.
2. Analyze the circuit using the saturation current-voltage relations.
3. Evaluate the resulting bias condition of the transistor. If the assumed parame-
ter values in step 1 are valid, then the initial assumption is correct. If
V
GS
< V
TN
, then the transistor is probably cutoff, and if
V
DS
< V
DS
(sat)
, the
transistor is likely biased in the nonsaturation region.
4. If the initial assumption is proved incorrect, then a new assumption must be
made and the circuit reanalyzed. Step 3 must then be repeated.
Additional MOSFET Configurations: DC Analysis
There are other MOSFET circuits, in addition to the basic common-source circuits
just considered, that are biased with the basic four-resistor configuration.
However, MOSFET integrated circuit amplifiers are generally biased with constant
current sources. Example 3.8 demonstrates this technique using an ideal current source.
3.2.3
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