ocw-ecc s13 introduction to field effect transistors...
TRANSCRIPT
Session 13
Introduction to Field Effect Transistors (FET)
Electronic Components and Circuits
Enrique San Millán / Celia López
Field Effect Transistors FET
OBJECTIVES• To know the structure of the device and the transistor • To know the structure of the device and the transistor
effect
• To know and distinguish different FET transistor types
• To understand the current-voltage characteristic of the device
• To identify the operating regions
Cut-off, Saturation, Ohm (triode)Cut-off, Saturation, Ohm (triode)
• To analyze FET circuits basic cases in DC
• To know small-signal model for FET transistors
2UC3M 2010 CCE - Session 13
Field Effect Transistors (FET)
Types Mode Channel
MOSFET(Metal-Oxide Semiconductor FET)
Enhancement/Accumulation
Channel N (or N-MOS)Channel P (or P-MOS)
Depletion Channel N (or N-MOS)Channel P (or P-MOS)
JFET(Joint FET)
Junction Channel NChannel P
Unipolar: only one carrier type (electrons in N-channel and holes in P-channel)
Basic characteristics
3
channel)
Control of Current (I) through Voltage (V) (BJT devices control I through I)
Three terminals:
Source (S): provides carriers
Gate (G): controls carriers flow
Drain (D): receives carriers
UC3M 2010 CCE - Session 13
Structure of Channel-n
Enhancement MOS Transistor D G S
MetalOxide (SiO2)
W
Drain (D)Gate (G) Source (S)
Metal Oxide (SiO2)
n+ n+Channelregion
Lp-typesubstrate
(Body) B
p-typesubstrate
(Body)
Drainregion
Sourceregion
n+ n+
Channelregion
L
4
D
S
BG
D
S
BG
D
S
G
D
S
G B
Body (B)
UC3M 2010 CCE - Session 13
n-MOS Transistor OperationG
DS
VGS
inducedn-type
channel
p-type substrate
B
GND
e-
e- e-
e-
+u +u
G
DS
VGS
VDS
iD iG = 0 iS =iD
5
p-type substrateB
GND
inducedn-type channel
+u +u
iD
UC3M 2010 CCE - Session 13
n-MOS Operation: Triode regioniD (mA)
0,4
0,3
vGS = Vt+2 V
vGS = Vt+1,5 V
G
DS
VGSVDS (small)
iD iG = 0iS =iD
vDS (mV)
0,2
0,1
0 50 100 150 200
vGS ≤ Vt
vGS = Vt+0,5 V
vGS = Vt+1 V
6
p-type substrate
B
GND
inducedn-type channel
+u +u
iD
UC3M 2010 CCE - Session 13
n-MOS Operation: Saturation regioniD
SaturationTriode
vDS<vGS - vt vDS ≥ vGS - vt
G
DS
VGS
VDS
iD iG = 0iS =iD
vDS
vGS > vt
vDSsat = vGS - vt
7
p-type substrate
B
GND
n-channel
+u +u
iD
UC3M 2010 CCE - Session 13
Current-Voltage Characteristic
VDS
+
-
iDiG = 0
Saturation regionTriode
region
vDS<vGS - vt vDS ≥ vGS - vt
iD (mA)
2,0 v = V +2,0
Triode region
[ ]2−−=
VGS
+
-
-
iD = iSvDS= vGS - vt
vDS (V)
1,5
2,0
1,0
0,5
0 1 2 3 4
vGS ≤ Vt (cutoff)
vGS = Vt+0,5
vGS = Vt+1,0
vGS = Vt+2,0
vGS = Vt+1,5
8
[ ]2)(2 DSDStGSD VVVVKi −−=
2)( tGSD VVKi −=
Saturation region (ID does not depend on VDS)
L
WCK oxnµ
2
1=
UC3M 2010 CCE - Session 13
Output Characteristics: Saturation
iD (mA)
2,0
1,5
1,0
0,5
0 0,5 1 1,5 2 2,5 3
vDS ≥ vGS - vt
9
2)( tGSD VVKi −=
Saturation region (ID does not depend on VDS)
vGS (V)vt
UC3M 2010 CCE - Session 13
Current-Voltage CharacteristicSaturation regionTriode
regioniD
vGS = Vt+2,0V
Slope = 1/ro
vDS
vGS ≤ Vt (cutoff)
vGS = Vt+0,5V
vGS = Vt+1,0V
vGS = Vt+1,5V
-VA = -1/λ
10
)1()(2
DStGSD VVVKi λ+−=
VA is the channel modulation voltage, producing a similar effect to the Early voltage in BJT
devices.
If we consider this effect then:
vGS ≤ Vt (cutoff)
UC3M 2010 CCE - Session 13
p-channel MOSFET (P-MOS)
Drain (D)Gate (G) Source (S)Source (S) Gate (G) Drain (D)
Polysilicon GateOxide
Thick
In enhancement p-mos there is a
channel if: 0<≤ VV
p+ p+
p-type body
S
BG
S
BG
S
G
n+ n+
n-well
ThickSiO2
(isolation)
11
channel if:
triode region
saturation region
0<≤ tGS VV
tGSDS VVV −≥
tGSDS VVV −≤S D DS
D
G B
UC3M 2010 CCE - Session 13
Depletion MOSFET
Equivalent behavior to enhancement MOSFET devices, except for
Manufactured channel:
When VGS<0 channel is reduced (e- leave Gate region)
When channel disappears (cut-off region)0<≤ VV When channel disappears (cut-off region)0<≤ tGS VV
D
S
BG
D
S
G
Saturation regionTrioderegion
vDS= vGS - vt
vDS<vGS - vt
vDS ≥ vGS - vt
iD (mA)
24
32
20
28
vGS = 2V (Vt+6)
vGS = 1V (Vt+5)
36
12
S
D
G B
vDS (V)
16
8
0 4 8 12
vGS ≤ -4 V (Vt)
vGS = -3V (Vt+1)
2 6 10 14
12
4vGS = -2V (Vt+2)
vGS = 0V (Vt+4)
vGS = -1V (Vt+3)
UC3M 2010 CCE - Session 13
Summary
In enhancement n-MOS there is a
channel if:
in triode region
in saturation region
0>≥ tGS VV
tGSDS VVV −≤
tGSDS VVV −≥
In enhancement p-MOS there is a
channel if:
in triode region
in saturation region
0<≤ tGS VV
tGSDS VVV −≥
tGSDS VVV −≤in saturation regiontGSDS VVV −≥ in saturation region
tGSDS VVV −≤
iD
0 vGS
n-channel enhancement
p-channel enhancement
p-channel depletion
n-channel depletion
13
In depletion n-MOS there is a
channel if:
in triode region
in saturation region
0, <≥ ttGS VVV
tGSDS VVV −≤
tGSDS VVV −≥
In depletion p-MOS there is a
channel if :
in triode region
in saturation region
0, >≤ ttGS VVV
tGSDS VVV −≥
tGSDS VVV −≤
0 vGS
UC3M 2010 CCE - Session 13
Junction Field Effect Transistor (JFET)
N channel P channelDrain
Gate
p-t
yp
e
Ga
te
n-type
Ch
an
ne
l
Drain
Gate
n-t
yp
e
Ga
te
p-type
Ch
an
ne
l
Drain
Gate
Gate
Drain
22/,)( pDSSpGSD VIKVVKi =−=
2
1
−=
p
GSDSSD
V
VIi
SourceSource
Gate
Source
Saturation regionTriode region
vDSsat= vGS - vp
vGS0 = 0
vGS1 = VGS0
Saturation
IDSIDS
Source
14
vGS4 < VP
vGS3 < VGS2
vGS2 = VGS1
Cutoff region
Saturation
region
Triode
region
vGS vp
VDSCutoff region
UC3M 2010 CCE - Session 13
DC bias point:
Load line
SaturationTriodeID v = V
VDD
v1 +
vo = vDS
vGS=v1 -
RD
SaturationTriodeID
IDQ
Q
Load line slope = -1/RD
v = V
vGS = V1B
vGS < V1B
vGS > V1B
vGS = VDD
B
C
15
vGS=v1 -
vDS =vo0 VOB=VIB-VIt
vGS = …
vGS = V1Q
A
VDDVOC VOQ=VDSQ
UC3M 2010 CCE - Session 13
FET transistor as amplifier:
VDD
voQ1
in triode region
Q1 in
saturation
Q1
cutoff
AVDD
Q
B
C
X
TimeVOQ=VOQ
VOB
V
vO
Slope at Q = voltage gain
16
VDD
VOC
Vt VIB=VOB+VtVIQ vivi
UC3M 2010 CCE - Session 13
Small-signal model
+
vgs gmvgs
G D
+
vgs gmvgs
G D
ro
SaturationTriode
iD
vGS = Vt+2,0V
SaturationTriode
vDS= vGS - vt
vDS<vGS - vt vDS ≥ vGS - vt
iD (mA)
1,5
2,0 vGS = Vt+2,0
-
vgs gmvgs
S
-
vgs gmvgs
S
ro
17
Slope = 1/ro
vDS
vGS ≤ Vt
(cutoff)
vGS = Vt+0,5V
vGS = Vt+1,0V
vGS = Vt+2,0V
vGS = Vt+1,5V
-VA = -1/λ
vDS= vGS - vt
vDS (V)
1,5
1,0
0,5
0 1 2 3 4
vGS ≤ Vt (cutoff)
vGS = Vt+0,5
vGS = Vt+1,0
vGS = Vt+1,5
UC3M 2010 CCE - Session 13
Small-signal parameters
+
-vgs gmvgs
G D
ro
)(2 tGS
VvGS
Dm VVK
V
ig
DSQds
−=∂
∂=
=
In MOSFETs
In JFETs
-
SiD
ID
An almost linear segment Slope = gm
id
tQ
18
−−=
∂
∂=
= p
GS
p
DSS
VvGS
Dm
V
V
V
I
V
ig
DSQds
12
In JFETs
0 vGSvt
vgs
vOV
t
UC3M 2010 CCE - Session 13
Small-signal parameters
+v g v
G D
r
A
DD
DS
D
o V
II
v
i
r=≈
∂
∂= λ
1
+
-vgs gmvgs
S
ro
SaturationTriode
Slope = 1/r
iD
vGS = Vt+2,0V
19
D
Ao
I
Vr =
Slope = 1/ro
vDS
vGS ≤ Vt
(cutoff)
vGS = Vt+0,5V
vGS = Vt+1,0V
vGS = Vt+1,5V
-VA = -1/λ
UC3M 2010 CCE - Session 13
Exercise:Operation regions. Saturation
EXAMPLE
|Vt| = 2 V
L=10um
W=100um
λ=02
/20 VuAC oxn =µ
VDD= 10 V
VD
R
ID
20
a) Design the circuit in order to obtain a ID=0.4mA
b) Calculate the value of R and voltage VD for that value of current
UC3M 2010 CCE - Session 13
Exercise:Operation regions. Triode region
EXAMPLE
VDD = 5 V
K = 0.5 mA/V2
|Vt| = 1 V
VDD= 5 V
VD = 0,1 V
R
ID
21
a) Design the circuit for obtaining VD=0.1V
b) Calculate the equivalent resistance of the transistor in this case
UC3M 2010 CCE - Session 13
Proposed exercise
ExampleVDD= +10V
K = 0.5 mA/V2
|Vt| = 1 V
RG2 = 10 MΩ
RG1 = 10 MΩ
RS = 6 kΩ
RD = 6 kΩ
22
a) Analyse this circuit and calculate the voltage in every node and the current in every line
b) Obtain the equivalent small-signal circuit
UC3M 2010 CCE - Session 13