Download Understanding MOSFET Amplifiers: Load Line Analysis & One-Supply Bias Circuit and more Slides Electrical Circuit Analysis in PDF only on Docsity!
FETs-
(Field Effect Transistors)
Learning Goals
- Understand the Basic Physics of MOSFET
Operation
- Describe the Regions of Operation of a
MOSFET
- Use the Graphical LOAD-LINE method to
analyze the operation of basic MOSFET
Amplifiers
- Determine the Bias-Point (Q-Point) for
MOSFET circuits
Load Line: Common Source Amp
- Using the values given the Schematic
- Now KVL on Right Loop
- Rearranging
- Of form: y = mx + b
- Using given values
vGS = 1V sin( [ 1000 ⋅ 2 π] t ) + 4 V
DD D D DS
DD D D DS or V R i v
V R i v = +
− + +
D
DS DD D
D (^) R v V R
i = −^1 +
20 (^ inmA)
1 k
20 V 1 k
1
D DS D
D DS i v i
i v or = − +
Ω
Ω
= −
Load Line: Common Source Amp
- Thus the LoadLine Equation
- Plot this on the FET vi Curve to determine the Operating Point
- Since this is a LINE need only 2-points - Intercepts are easy - Making a T-Table
Ω
Ω
= − 1 k
20 V 1 k
1 iD vDS
vDS i D
0 20 mA
20V 0
Max and Min Opp-Points
- The common source Amp is designed to Operate in the SATURATION Region. Recall the vGS Eqn
- By sin behavior
- Reading the vi-LL graph find (vDS ,iD ) co-ords - (vDS ,i (^) D ) (^) max = (4V,16mA) - vGS = 5V - (vDS ,i (^) D ) (^) min = (16V,4mA) - vGS = 3V
vGS = 1V sin ( 2000 π t ) + 4 V
1V 4 V 3V ( Pt-B)
1V 4 V 5V Pt-A ,min
,max =− + =
= + = GS
GS v
v
Voltage Swing
- The common source Amp is must stay in Saturation. For this nFET that means max & min vGS values of 5V & Vto given the 1V amplitude of the sin
- From Last Slide We calculated corresponding
Xmax/min values for vDS
- vDS,min = 4V (vGS = 5)
- vDS,max = 16V (vGS = 3)
- Note that the output direction is Opposite the Input direct
- The ckt produces a SATURATED output Voltage Swing of 4V-16V = −12V
LoadLine Gain
- Notice
- This is due to the NONlinear nature of MOSFETS; they are “Square-Law” devices - The i (^) D lines in SAT are not evenly Spaced
Input
Output
LoadLine Gain
- Since the FET is NOT linear, vout is NOT directly proportional to v (^) in , so we can NOT Define a true Gain
- “Small Signal” methods WILL allow us to define a true grain for the AC part of the voltage input - Requires Calculus - To “Linearize” ckt
Input
Output
Saturation Slippery-Slope
- Must also take care that the small-signal input
does NOT push the FET Out of Saturation at
ANY Time.
- The v (^) in -Amplitude and Bias-Pt Selection could
- Drive the FET out of SAT and into TRIODE Operation
- Drive the FET into CutOff (vGS < Vto)
One-Supply Bias Circuit
- Usually only ONE supply voltage is available. In this case set VG with a voltage divider
- By Thevenin - Since the Gate on a IGFET draws NO current, we have a simple voltage divider on the Left thru R 1 & R 2. - Thus VG to GND
G V DD
R R
R
V
1 2
2
1 2
1 2
1 || 2
R R
R R R
R R R
G
G
=
=
One-Supply Bias Circuit
- If the Circuit has been properly Biased the FET is in SATURATION
- In Saturation i D is independent of v DS and equals, at the operating , or Q, point - Recall the KVL eqn on the GATE Loop (now Assumed at the “Q” point): - Sub into SAT eqn
↓ i D
( ) 2 i (^) DQ = K vGSQ − V to
S
G GSQ DQ (^) R
V v i
−
( ) 2 GSQ to S
G GSQ K v V R
V v = −
−
One-Supply Bias Circuit
- Solve for vGSQ :
- Or:
- Introduce new Constant:
- Yields quadratic Eqn in v (^) GSQ :
- Now Solve by MATLAB’s MuPAD
( ) 2 GSQ to S
G GSQ K v V R
V v = −
−
( ) 2 V (^) G − vGSQ = RSK vGSQ − V to U = RS K
UvGSQ^2 + ( 1 − 2 UVto ) v (^) GSQ +( UV (^) to^2 − VG ) = 0
One-Supply Bias Circuit
- Discarding the Negative Root find
- Then Find iDQ by subbing vGSQ from above into
the gate KVL Eqn:
U
UV U V V v (^) GSQ to G to 2
2 − 1 + 4 − + 1
S
G GSQ DQ R
V v i
−
One-Supply Bias Circuit
- Solving the last two eqns yields iDQ and v (^) GSQ - Beware that the parabolic i (^) D eqn will produce an extraneous root - Discard the SMALLER root as SAT requires: vGS−Vto ≥ 0 - The KVL eqn on ckt Right-Side - ReArranging - Then with iDQ from before (MuPAD)
S D
D D DS
DD
R i
R i v
V
0 = − +
v (^) DS = VDD − ( RD + RS ) i (^) D
v (^) GS − Vto = ± iD K v^ DSQ = VDD −^ (^ RD + RS ) i^ DQ
iD ↓