3.Field-Effect Transistor (FET) Junction Field-Effect Transistor (JFET) n-channel JFET V

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3.Field-Effect Transistor (FET)
Junction Field-Effect Transistor (JFET)
n-channel JFET
VGS = 0 V and VDS positive value
When VGS=0V and C some positive value,the upper region of the p-type material will be reverse biased higher than the lower
region(the greater the reverse bias,the wider the depletion region).
As the voltage VDS is increased from 0 to a few volts,the current will increase as determined by Ohm’s law and The depletion region
will widen,causing a noticeable reduction in channel widht.If VDS is increased to a level where it appears that the two depletion
regions would “touch”, a condition referred to as pinch-off will result.The level of VDS that establishes this condition is referred to
as pinch-off voltage Vp (when VGS=0V and VDS>Vp IDSS).
Input resistance > 10 8 
VGS < 0V
Shockley’s Equation:
Voltage-Controlled Resistor:
where ro is the resistance with VGS _ 0 V and rd the resistance at a particular level of VGS.
Power dissipation:
p-channel JFET
PD = |VD|ID
Metal-Oxide-Semiconductor Field-Effect Transistor (MOSFET) Or Insulated-Gate FET (IGFET)
Depletio-Type MOSFET (D-MOSFET) n-channel D-MOSFET
When VGS=0V,the drain current is IDSS.
The negative potential at the gate will tend to pressure electrons toward the p-type substrate and attract holes
from the p-type substrate.The drain current is therefore reduce with increasing negative bias for VGS.
The positive potential at the gate will draw additional electrons (free carrier) from the p-type substrate due to
the reverse leakage current,reveals that the drain current will increase.
10
Input resistance > 10 
p-channel D-MOSFET
Enhachement-Type MOSFET (E-MOSFET)
n-channel E-MOSFET
If VGS = 0V,the absence of an n-channel will result in a
current of effectively zero amperes.
VD(ON)
VT
VGS(ON)
p-channel E-MOSFET
VGS
Complementary MOSFET (CMOS)
A very effective logic circuit can be established by contructing a p-channel and an n-channel MOSFET on the
same substrate.
FET Biasing
For de analysis,the coupling capacitors are open cicuits.
Fixed-Bias Configuration
Graphical Approach:
Self-Bias Configuration
Graphical Approach:
=-ID (1K
)
Voltage-Divinder Biasing
Graphical Approach:
Depletion-Type MOSFET
Graphical Approach:
Enhancement-Type MOSFET
Graphical Approach:
VGS  VDS  VDD  I D RD  12V  I D (2 K)
I D  0  VGS  12V
VGS  0  I D  6mA
I DQ  2.75mA
VGS  VDSQ  6.4V
p-channel FET
Graphical Approach:
 VGS  VG  I D RS  4.55V  I D (1.8K)
I D  0  VGS  4.55V
VGS  0  I D  2.53mA
FET Small-Signal Model
 V
I D  I DSS 1  GS
VP

g m  y fs 



2
2I
DI D
| VDS  const  DSS
DVGS
| VP |
At VGS Q   0.5V  g m 
 VGS
1 
VP


 V
  g mo 1  GS
VP





DI D
2 mA

 3.3mS
DVGS 0.6V
DI D
1.8mA

 2 .4 mS
DVGS 0 .75V
DI D
1.5mA
  2.5V  g m 

 1.4 mS
DVGS
1.1V
At VGS Q   1.5V  g m 
AtVGS Q
D
ID
ID
VGS
FET ac equivalent model:
Output resistance:
rd 
Input Impedance of the FET:
Z i (FET )  
(the typical values: JFET  109 , MOSFET  1012  1015 )
Output impedance of the FET:
Z o ( FET )  rd 
1
yos
DVDs
7V

 14k
DI D
0.5mA
FET Small-Signal Analysis
Common-Source Circuit
+VDD
FET ac equivalent model:
Output resistance:
+VDD
Vi = 0
Zo = RD ||rd
RD
C2
R1
C1
R2
Rs
Cs
Z i  R1 || R2
Vo  ( g mVgs )( RD || rd )  ( g mVi )( RD || rd )  Av 
Vo
  g m ( RD || rd )
Vi
+VDD
RD
rd  
Vgs  Vi  g mVgs Rs
 Vi  Vgs (1  g m Rs )
RG
Rs
Vo  ( g mVgs ) RD
Av 
Vo
g R
 m D
Vi
1  g m Rs
rd  
Vgs  Vi  I o Rs
D
I o  g mVgs 
Vi
Vo  Vs
I R I R
 g mVgs  o D o s
rd
rd
 g m (Vi  I o Rs ) 
Vo
 Io 
Vo  Vs
rd
Io
g mVi
( R  Rs )
1  g m Rs  D
rd
Vo   I o RD  
 Av 
 I o RD  I o Rs
rd
g m RDVi
( R  Rs )
1  g m Rs  D
rd
Vo
g m RD

( R  Rs )
Vi
1  g m Rs  D
rd
Common-Drain (Source-Follower) Circuit
Vo  g mVgs ( RS || rd )  g m (Vi  Vo )( RS || rd )  Av 
G
Vo
g m ( RS || rd )

Vi 2  g m ( RS || rd )
S
Z i  RG
Vi  0  Z o  RS || rd ||
Common-Gate Circuit
Vo  ( g mVgs ) RD   g m (Vi ) RD  AV 
Z i  RS ||
1
gm
Vi  0  Z o  RD || rd
Vo
 g m RD
Vi
1
gm
Enhancemen MOSFET Amplifier
k
I D (ON )
(VGS ( ON )  VTh ) 2
Vo  ( I1  g mVgs )( RD || rd )  (
2
(typically 0.3 mA/V )
Vi  Vo
 g mVi )( RD || rd )
RG
Vo (1  g m RG )( RD || rd )
 AV 

Vi
RG  RD || rd
(for g m RG  1)
(for RG  RD or rd

g m RG ( RD || rd )
  g m ( RG || RD || rd )
RG  RD || rd
  g m ( RD || rd )
Ii 
Vi  Vo

RG
Vi (1 
RG
Vo
)
Vi
 Zi 
Vi  0  RD || rd || RG  RD || rd
Vi
RG
RG
RG



I i 1  AV 1  ( g m ( RD || rd )) 1  g m ( RD || rd ))
System Approach-Effects of RS and RL
Bypassed Source Resistance
AV 
Unbypassed Source Resistance
Source Follower
Vo
  g m ( R L || R D )
Vi
Common Gate
AV 
Vo
 gm(RL || RD)
Vi
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