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Lecture 18 ANNOUNCEMENTS HW#10 will be posted tonight OUTLINE HW#10 will be posted tonight OUTLINE Basic MOSFET amplifier MOSFET bi i MOSFET biasing MOSFET current sources C lifi Commonsource amplifier EE105 Fall 2007 Lecture 18, Slide 1 Prof. Liu, UC Berkeley Reading: Chapter 7.17.2

Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

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Page 1: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

Lecture 18

ANNOUNCEMENTS• HW#10 will be posted tonight

OUTLINE

• HW#10 will be posted tonight

OUTLINE• Basic MOSFET amplifierMOSFET bi i• MOSFET biasing

• MOSFET current sourcesC lifi• Common‐source amplifier

EE105 Fall 2007 Lecture 18, Slide 1 Prof. Liu, UC Berkeley

Reading: Chapter 7.1‐7.2

Page 2: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

Basic MOSFET Amplifier

• For large small‐signal gain, the MOSFET should be operated in the saturation region.

EE105 Fall 2007 Lecture 18, Slide 2 Prof. Liu, UC Berkeley

Vout should not fall below Vin by more than VTH.  

Page 3: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

MOSFET BiasingThe voltage at node X is determined by VDD, R1, and R2:Also

DDX VRR

RV21

2

+=

RIVV +=Also, SDGSX RIVV +=

( )21THGSoxnD VVWCI −= µ

( ) THDD

THGS VRR

VRVVVVV 2 21

211 ⎟

⎞⎜⎜⎝

⎛−

+++−−=⇒

( )2 THGSoxnD VV

LCµ

SRWCV

RR

µ

1 where 1

21

=

⎠⎜⎝ +

EE105 Fall 2007 Lecture 18, Slide 3 Prof. Liu, UC Berkeley

Soxn RL

Page 4: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

Self‐Biased MOSFET Stage• Note that there is no voltage dropped across RG

M1 is operating in the saturation region.M1 is operating in the saturation region.

DDDSGSDD VIRVRI =++

EE105 Fall 2007 Lecture 18, Slide 4 Prof. Liu, UC Berkeley

Page 5: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

MOSFETs as Current Sources• A MOSFET behaves as a current source when it is operating in 

the saturation region.g• An NMOSFET draws current from a point to ground (“sinks 

current”), whereas a PMOSFET draws current from VDD to a point (“sources current”)point ( sources current ).

EE105 Fall 2007 Lecture 18, Slide 5 Prof. Liu, UC Berkeley

Page 6: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

Common‐Source Stage: λ = 0Amplifier circuit Small-signal analysis circuit

for determining voltage gain, Av

RIWCRgA == µ2

Small-signal analysis circuit fordetermining output resistance, Rout

in

DDoxnDmv

R

RIL

CRgA

∞=

−=−= µ2

EE105 Fall 2007 Lecture 18, Slide 6 Prof. Liu, UC Berkeley

Dout RR =

Page 7: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

Common‐Source Stage: λ ≠ 0• Channel‐length modulation results in reduced small‐signal 

voltage gain and amplifier output resistance.g g p p

Small-signal analysis circuitfor determining voltage gain, Av

Small-signal analysis circuit fordetermining output resistance, Rout

( )||( )in

ODmv

RrRgA

||

||∞=−=

EE105 Fall 2007 Lecture 18, Slide 7 Prof. Liu, UC Berkeley

ODout rRR ||=

Page 8: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

CS Gain Variation with L• An ideal current source has infinite small‐signal resistance.The largest Av is achieved with a current source as the load. g v

√• Since λ is inversely proportional to L, Av increases with √L.  

Doxn WLCILWC µµ 22

EE105 Fall 2007 Lecture 18, Slide 8 Prof. Liu, UC Berkeley

D

oxn

Domv I

WLCI

LrgA µλ

2∝==

Page 9: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

CS Stage with Current‐Source Load• Recall that a PMOSFET can be used as a current source from VDD.

Use a PMOSFET as a load of an NMOSFET CS amplifier.Use a PMOSFET as a load of an NMOSFET CS amplifier.

( )211

|||| OOmv

rrRrrgA

=−=

EE105 Fall 2007 Lecture 18, Slide 9 Prof. Liu, UC Berkeley

21 || OOout rrR =

Page 10: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

PMOS CS Stage with NMOS Load • An NMOSFET can be used as the load for a PMOSFET CS amplifier. 

212 )||( OOmv rrgA −=

21

212

|| OOout

OOmv

rrR =

EE105 Fall 2007 Lecture 18, Slide 10 Prof. Liu, UC Berkeley

Page 11: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

CS Stage with Diode‐Connected LoadAmplifier circuit Small-signal analysis circuit

including MOSFET output resistances

:0≠λ

( )1/1

:0 If

LWA

=λ12

21 ||||1

OOm

mv rrg

gA ⎟⎟⎠

⎞⎜⎜⎝

⎛−=

A i l b t it i l d d t t

( )( )2

1

21 /LWg

gAm

mv −=⋅−=12

2

||||1OO

mout rr

gR =

EE105 Fall 2007 Lecture 18, Slide 11 Prof. Liu, UC Berkeley

Av is lower, but it is less dependent on process parameters (µn and Cox and drain current (ID).

Page 12: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

CS Stage with Diode‐Connected PMOS Load

1 ⎞⎜⎛

:0≠λ

211

2

1

||||1oo

mmv rr

ggA ⎟

⎞⎜⎜⎝

⎛−=

211

||||1oo

mout rr

gR =

EE105 Fall 2007 Lecture 18, Slide 12 Prof. Liu, UC Berkeley

Page 13: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

CS Stage with DegenerationAmplifier circuit Small-signal analysis circuit

for determining voltage gain, Av

S

Dv

Rg

RA+

−== 1 :0 If λ

EE105 Fall 2007 Lecture 18, Slide 13 Prof. Liu, UC Berkeley

mg

Page 14: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

Example• A diode‐connected device degenerates a CS stage.

11D

v

gg

RA+

−=

EE105 Fall 2007 Lecture 18, Slide 14 Prof. Liu, UC Berkeley

21 mm gg

Page 15: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

Rout of CS Stage with Degeneration• Degeneration boosts the output impedance:

Small-signal analysis circuit fordetermining output resistance, Rout

Current flowing down through r isCurrent flowing down through ro is

( )SXmX

SXmXmX

RigiRigivgi

+=−−=−

1

( )SX Riv −=1

SXmX g

( )

( )X

XSXSXmXO

RrgrRRgrvvRiRigir

+≅++

=++

1

EE105 Fall 2007 Lecture 18, Slide 15 Prof. Liu, UC Berkeley

( ) SOmOSSmOX

X RrgrRRgri

+≅++= 1

Page 16: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

Output Impedance Examples

⎞⎛ 1⎟⎟⎠

⎞⎜⎜⎝

⎛+≅

211

11m

mOout ggrR 1211 OOOmout rrrgR +≈

EE105 Fall 2007 Lecture 18, Slide 16 Prof. Liu, UC Berkeley

Page 17: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

CS Stage with Gate Resistance• For low signal frequencies, the gate conducts no current.

Gate resistance does not affect the gain or I/O impedancesGate resistance does not affect the gain or I/O impedances.

EE105 Fall 2007 Lecture 18, Slide 17 Prof. Liu, UC Berkeley

Page 18: Lecture 18 - University of California, Berkeleyee105/fa07/lectures... · 2007. 11. 2. · Lecture 18 ANNOUNCEMENTS • HW#10 will be posted tonight OUTLINE will be posted tonight

CS Core with Biasing

Dv

RRRR

RRA −⋅

+= 1||

|| 21Dmv Rg

RRRRRA 21

||||

−=S

m

G Rg

RRR ++ 1|| 21Dm

Gv g

RRR 21 ||+

EE105 Fall 2007 Lecture 18, Slide 18 Prof. Liu, UC Berkeley