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HKN ECE 342 Review Session 2 HKN ECE 342 Review Session 2

HKN ECE 342 Review Session 2 - PowerPoint Presentation

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HKN ECE 342 Review Session 2 - PPT Presentation

Anthony Li Milan Shah MOSFETs NMOS PMOS MOSFET Operating Point Three regions of operation Cutoff V G lt V T I D 0 LinearTriode V G gt V T V DS lt V GS V ID: 724850

common tied transistor diode tied common diode transistor source drain transconductance degeneration modulation midterm problem regions resistance operation gain

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Slide1

HKN ECE 342 Review Session 2

Anthony Li

Milan ShahSlide2

MOSFET’s

NMOS

PMOSSlide3

MOSFET Operating Point

Three regions of operation:

Cutoff (V

G

< VT

): ID = 0Linear/Triode (VG > VT, VDS < VGS - VT):

Saturation (V

G

> VT, VDS > VGS - VT): Note:

 Slide4

MOSFET Incremental Model

Transconductance:

 Slide5

Gain Calculation

A

v

= -G

MRoutG

M = Small signal transconductance, ratio of iout to vin ROUT = Equivalent incremental output resistanceSlide6

Common Amplifier Topologies

Diode-tied Transistor

Common Source/Drain/Gate

Common Source with Degeneration

Common Drain with Modulation

CascodeDiode Tied TransistorSlide7

Diode-Tied Transistor

R

OUT

=

for

or

 

Diode Tied TransistorSlide8

Common Source/Drain/Gate

 

 

 Slide9

Degeneration

When a resistance is “viewed” through the drain, it appears bigger by a factor related to the transconductance.

 Slide10

Modulation

Resistances seen through the source seem smaller:

for g

m

r

ds

>> 1

 

 Slide11

Cascode

 

 Slide12

BJTSlide13

Regions of Operation

Three regions of operation:

Cutoff: V

E

> VB < VC

Saturation: VE < VB > VCForward Active: VE > VB > VC

V

T

= kt/qIC = ꞵIBIE = IC + IBꞴ = gmR𝜋Slide14

BJT Small Signal ModelSlide15

Terminal Impedance

R

C

=

ro

RB = RℼRE =

Diode-Tied =

 Diode Tied TransistorSlide16

Common Emitter/Collector/Base

 

 

 Slide17

Degeneration

When a resistance is “viewed” through the collector, it appears bigger by a factor related to the transconductance.

R

IN

= R

B

+R

𝜋

+(ꞵ+1)RE Slide18

Modulation

Resistances seen through the Emitter seem smaller.

 Slide19

Bode Plots

Magnitude

Pole: Roll down by 20

db

/dec, 6 db/oct

Zero: Roll up by 20 db/dec, 6 db/octPhase: arctan(ω/ωp)Usually -90° for poles, +90° for zeros

ω

ugf

= 20log|An| * ωpn where n is the pole located before unity gain frequencySlide20

Miller Effect

 Slide21

Problem 1: Midterm 3 Fa17Slide22

Problem 2: Midterm 2 Fa16 Slide23

Problem 3: Midterm 2 Fa16

A.

,

B. Refer to solutions