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1 BJT and MOSFET characteristics and Op-Amps Prof K.N.Bhat, ECE Department , IISc Bangalore email: [email protected] Micro and Smart Systems Lecture -32

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Page 1: Micro and Smart Systems - NPTEL

1

BJT and MOSFET characteristics and Op-Amps

Prof K.N.Bhat,

ECE Department , IISc Bangalore

email: [email protected]

Micro and Smart Systems

Lecture -32

Page 2: Micro and Smart Systems - NPTEL

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Topics for Discussion • BJTs , MOSFETs and CMOS

•Amplifiers and Op Amp Concepts

• Basic Op-Amp circuits

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Bipolar Junction Transistor (BJT)

RVI I 0

PNHole collection, I0

EV

IP N

Hole injection E

T

VI I exp( )V

0

Forward Biased Junction Reverse Biased Junction

Hole injectionE

E ET

VI I exp( )V

0 Hole collection, Cp EI I

C Cp C E CI I I I I 0 0

EV

EI P N

RV

PCIPNP Transistor

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P+ N PEI

CI

BI

PNP Transistor

pEI pCI

CI 0

EBV CBV

C pC co E coI I I I I

( )

1C B CI I ( )I 01

E

B

C

E

B

C

C CB E C C C C

I II I I I I I

0

01 1

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N+ P NEI

CI

BI

C nC co E coI I I I I

nCInEI

CI 0

C B CI I ( )I 01 ( )

1

NPN Transistor

BEV CBV

E

B

C

C

B

E

Note that the voltage polarities and the current flow directions in NPN transistors are exactly opposite to that of PNP transistors

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Common Base Characteristics

C E coI I I

Saturation Region

Active Region

Cut off Region

is very close to 1.0 but always < 1

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OB

IC A

Output Characteristics of a BJT(Common Emitter configuration)

coI ( ) 1 VCE

C B CI I ( )I 01

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Metal Oxide Semiconductor Field Effect Transistor (MOSFET)

P- Silicon

VGS=0 +VDS

N+ N+ID= 0

P- SubstrateN+ N+

SourceGate

Drain

Device structure VGS = 0 VDS > 0

ID

P- Silicon

+VGS +VDS

N+ N+

VGS > Threshold Voltage, Vth

VDS

IDVGS3

VGS2

VGS1VGS=Vth

ID –VDS is linear when VDS is small

VGS3 > VGS2 > VGS1 > Vth

S D

S D

Page 9: Micro and Smart Systems - NPTEL

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MOSFET Characteristics

ID

P- Silicon

+VGS +VDS

N+ N+

VDS < (VGS-Vth) . ID –VDS is non linear

ID

P- Silicon

+VGS +VDS

N+ N+

VDS > (VGS-Vth). ID Saturates

VGS=2V

VGS=Vth

Triode region

Saturation region

IDVDS=VGS-Vth

Cut off region

VGS = 3V

VGS = 4V

D( sat ) GS thI K(V V ) 2

DSD GS th DS

VI K [(V V )V ]

22

2

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MOSFET types

ID

P- Silicon

+VGS +VDS

N+ N+

N-ChannelDB

S

G

N - Channel

ID

N- Silicon

-VGS -VDS

P+ P+

P-ChannelDB

S

G

P - Channel

Transfer Characteristics

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Complementary MOS (CMOS) Inverter Circuit

High1

Low0

Low0

High1

iV oV

N- channel MOSFET

P- channel MOSFET

VDD

iV oV

S

S

D

D

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Amplifiers• Output of transducers are in the range µV or mV and possess very low energy .

• Signal processing is easier if signal is large in the range of Volts

vo

vin

o ov

in in

v vAv v

ov

in

vAv

Voltage Gain

Transfer Characteristics

iinAmplifierOne or more

Amplifying DevicesVin

+-

+-

vo

io

Current Gain oI

in

iAi

o 0p v I

in in

v iA A Av i

Power Gain

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Logarithmic Gain

The amplifier gains Av, AI and Ap are usually very large and extend over several orders of magnitude . They are normally expressed in terms of logarithms (in decibels) as follows:

Power Gain in dB= 10 log Ap=10 log10(P0/PI )

Voltage gain in dB = log ( ) log ( )2o o

10 102inin

v v10 20vv

Current Gain in dB = log ( ) log ( )2o o

10 102inin

i i10 20ii

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Input and Output Resistance

Input Resistance Ri is a measure of the current drawn by the amplifier .

ini

in

VRI

Output Resistance Ro is the internal resistance seen from the output terminals (A and B) of an amplifier . It is the Thevenin’s equivalent resistance looking into the amplifier

iinAmplifierOne or more

Amplifying DevicesVin

+-

A

BRo

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DC Power Supplies for the amplifierThe DC power supply is required to set up the operating point so that the ac signal can be superimposed as shown below along with the symbol for the amplifier

This allows variation in output signal in response to a small change in the input signal

VDC

vac RL sino o mv V v t

The DC supply (or supplies ) provides the power delivered to the load and the power dissipated as heat within the amplifier .

vo

Vin

Vo Time

Small signal

VDC

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BJT Amplifier (common Base )

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EB

T

VV

E oI I e

E E

BE e T

I I1V r V

Te

E

V 25mVr 25I 1mA

Incremental Resistance re of the Junction

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= 4VVC

Maximum Vo swing is 2Vpeak and then it will get saturated

VBC=2V

Example: RL=1K, VC=4V. Then IC=2mA, VBC=2V.

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Operational Amplifiers

• The Operational Amplifier (or op-amp) is a high–gain, direct coupled amplifier operates with a Differential Voltage between two input terminals

• The symbol for op-amp is as shown

• It and consists of Multiple stages :

(1) An input stage to provide high input resistance and certain amount of voltage gain

(2) Middle stages to provide a high voltage gain

(3) An output stage to provide a low output resistance

and has at least Five terminals

VS+

VS

v+

v-

+v0

2

3

7

4

6

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Op Amp Terminals

Symbol and terminals of Op-Amp

VS+

VS

v+

v-

+v0

2

3

7

4

6

Terminal 2 is “Inverting input” . The output that results from input at this terminal will be inverted .

Terminal 3 is “Non-inverting input”. The output that results from input at this terminal will have the same polarity as input

Terminals 4 and 7 are respectively negative and positive DC pwer supplies VS- and VS+ respectively

Terminal 6 is the output terminal

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The output Voltage Vo of the op-amp is related to the open loop gain and the difference voltage

Op-amp equivalent circuit and ideal model

( )0 o d oV A V A V V oA dV

Equivalent Circuit

+

Vo

Ro

Ri AoVd

+

-

V+

V-

-

V S+

V S-

Model of Ideal Op ampV+

V- -+ Vo =AoVd

+

-dV 0

, ,i o oR R 0 A

Typical values of Ro =75

Op-amps with MOSFET have Ri=1012

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VS

Slope = A0

v0

Vd

VS+

Op-amp transfer Characteristics (Vo versus Vd)

•Vo versus Vd is almost linear for small values of Vd .

• As Ao is very arge the Vo saturates when it exceeds positive and negative values

• is set by the supply voltages of the op amp and is usually about 1 Volt below them.

satV

satV

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Basic Op amp CircuitsInverting Amplifier

-

Consider the ideal model :,o iA R

d inV 0 and i 0

. ( )d AV 0 V 0 1 . ( )in 1 2i 0 i i 2

-+ Vo

VS

VAR1

R2

ini

1i

2i

From (1) and (2) s o

1 2

V VR R

2o s

1

RV VR

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Non-inverting AmplifierR2

-+ VoVS

VAR1 ini

1i

2iConsider ideal op-amp

VA=VS and i1=12

1S o

1 2

RV VR R

1 2o S

1

R RV VR

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Other configurations of the Op-amp

-+ VoVS

1. Voltage Follower. Buffer stage between two stages to prevent loading

C

-+ Vo

VS

R

1i

2i

2.Integrator: To generate Saw tooth from square wave.

( )o s1V V t dt

RC

3. Differentiator: To generate square wave from triangular wave

-+ Vo

VS

C

R

1i

2i

o SV V

So

dVV RCdt

o2

dVi Cdt

S1

ViR

1 2i i

S1

dVi Cdt

o2

ViR

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R2

-+ Vo

V2VA

R1

V1 R1

R2

VB

R2

Vo2

-+V2

R1-+ Vo1VB

R1

R2

Op-amp Differential Amplifier

( )4B 1

3 4

RV V 1R R

( )20 o1 o2 1 2

1

RV V V V VR

( )2 2B 1

1o

11

R RV 1 VR

VR

2o22

1

RVVR

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Instrumentation Amplifier

rg S1 S2rg

g g

V V ViR R

VS1

VS2

( )rg S1 S2V V V

R2

-+ Vo

R1

R1R2

R

R

Rg

-+

-+

A1

A2

A3rgiV1

V2

( ) ( )S1 S2d 1 2 g

g

V VV V V 2R RR

( )( )2 2o d S1 S2

1 g 1

R R2RV V V V 1R R R

Dedicated Differential Amplifier with very high input Resistance . Its gain can be adjusted with a single resistance Rg

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Merits of Instrumentation Amplifier

• Extremely High Input impedance.

•High Common Mode Rejection Ratio (CMRR) (ie. It is bale to reject a signal that is common to both terminals but to amplify a differential signal )

•The high CMRR is very useful for receiving very small signals buried in large common-mode offsets or noise

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Instrumentation Amplifier with Fixed GainR2

VS1

VS2

-+ Vo

R1

R1R2

-+

-+

A1

A2

A3

( )d S1 S2V V V

+

-( )2

o S2 S11

RV V VR