Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

43
Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS Prepared by Engr:Sarfaraz Khan Turk Lecturer at IBT LUMHS Jamshoro

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Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS. Prepared by Engr:Sarfaraz Khan Turk Lecturer at IBT LUMHS Jamshoro. Basic BJT Amplifiers Circuits. Single-Stage BJT Amplifiers. Key Words : Common-Emitter Amplifier Graphical Analysis Small-Signal Models Analysis - PowerPoint PPT Presentation

Transcript of Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Page 1: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Lecture no 2 to 5

THE BASIC BJT AMPLIFIER CONFIGURATIONS

Prepared by Engr:Sarfaraz Khan Turk

Lecturer at IBT LUMHS Jamshoro

Page 2: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Single-Stage BJT Amplifiers

Key Words: Common-Emitter Amplifier Graphical Analysis Small-Signal Models Analysis Common-Collector Amplifier Common-Base Amplifier

Page 3: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

C-E AmplifiersTo operate as an amplifier, the BJT must be biased to operate in active mode and then superimpose a small voltage signal vbe to the base.

oC

CER

cii

BBEC

i vviivv CBC 12

DC + small signal

OC vi Bi iv CB ii

coupling capacitor (only passes ac signals)

Page 4: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

C-E Amplifiers

iV

iV

Vi

+

iV

Page 5: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

C-E Amplifiers

vBE=vi+VBE

bBB iIi

Apply a small signal input voltage and see ib

Page 6: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Single-Stage BJT AmplifiersC-E Amplifiers

• vi = 0 IB 、 IC 、 VCE

ceCECE

CCC

bBBi

vVviIi

iIiv 0

)()( ioiMoM ffVV •

• vo out of phase with vi

iC=ic+IC

vCE=vce+VCE

See how ib translates into vce.

Page 7: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

C-E Amplifiers Considering (all the capacitors are replaced by open circuits)

CV

Considering (all the capacitors are replaced by short circuits)

iV

Page 8: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Single-Stage BJT AmplifiersC-E Amplifiers

Considering (all the capacitors are replaced by open circuits)

CV

Considering (all the capacitors are replaced by short circuits)

iV

Page 9: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Single-Stage BJT AmplifiersGraphical Analysis

VCC

• Can be useful to understand the operation of BJT circuits.• First, establish DC conditions by finding IB (or VBE)• Second, figure out the DC operating point for IC

Can get a feel for whether the BJT will stay in active region of operation – What happens if RC is larger or smaller?

Page 10: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Graphical Analysis

VCC

')//( LcLCcce RiRRiv

Page 11: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Single-Stage BJT AmplifiersGraphical Analysis

Q-point is centered on the ac load line:

VCC

Page 12: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

VCC

Basic BJT Amplifiers Circuits

Single-Stage BJT AmplifiersGraphical Analysis

Clipped at cutoff(cutoff distortion)

Q-point closer to cutoff:

Page 13: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

VCC

Basic BJT Amplifiers Circuits

Single-Stage BJT AmplifiersGraphical Analysis

Clipped at cutoff(saturation distortion)

Q-point closer to saturation:

Page 14: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Graphical Analysis

Page 15: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Small-Signal Models Analysis

Steps for using small-signal models1. Determine the DC operating point of the BJT - in particular, the collector current2. Calculate small-signal model parameters: rbe

3. Eliminate DC sources – replace voltage sources with short circuits and current sources with open circuits4. Replace BJT with equivalent small-signal models5. Analysis

Page 16: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Small-Signal Models Analysis

IC ≈ βIB, IE = IC + IB = (1+β)IB

eEBEbBCBC RIVRIR)II(V

))(1( eb

BECB RRR

VVI

)( eECCCCE RRIRIVV

Example 1

Page 17: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Small-Signal Models Analysis

Example 2

vs

CCbb

bB V

RRRV

21

2

eBe

BEBEC RV

RVVII /

C

BII

)RR(IVV eCCCCCE

Page 18: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Single-Stage BJT AmplifiersSmall-Signal Models Analysis

There are three basic configurations for single-stage BJT amplifiers: – Common-Emitter – Common-Base – Common-Collector

VBB VCCRC

NN P ce

b

(a)

VBB VCC

RcN

NP

c

e

b

(b)

VBB

VCC

Re

N

NP

c

e

b

(c)

E B CV V V E B CV V V E B CV V V

Page 19: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Common-Collector Amplifier

eEBEbBCC RIVRIV eBBEbB RIVRI )1(

eb

CC

eb

BECCB RR

VRR

VVI

1)1(

BC II

eCCEeECECC RIVRIVV

eCCCCE RIVV

(a) 共集电极电路

Note : is slightly less than due to the voltage drop introduced by

oV iV BEV1VA

Page 20: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Common-Collector Amplifier

(a) 共集电极电路

The last basic configuration is to tie the collector to a fixed voltage, drive an input signal into the base and observe the output at the emitter.

Page 21: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Common-Collector Amplifier

)//()]//)(1([ LeebebLebebi RRIrIRRrIV

)//)(1()//( LebLeeo RRIRRIV

1)//)(1(

)//()//)(1(

)//)(1(

Lebe

Le

Lebe

Le

i

OV RRr

RRRRr

RR

V

VA

Let’s find Av , Ai :

Page 22: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Common-Collector Amplifier

bbiLebeb RIIRRrI )())//)(1((

b

bLeb

b

bLebebi R

RRRIR

RRRrII

)//)(1()//)(1(

L

Lebo R

RRII )//)(1(

bLe

b

L

Lei RRR

RR

RRA

)//)(1(

)//)(1(

L

Le

RRR )//)(1(

)//)(1( Le RR << Rb

iAL

Le

RRR )//)(1(

>>1

Let’s find Av , Ai : )//()1()//( LebLeeLo RRIRRIRI

oI

iI

Page 23: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Common-Collector Amplifier

Ri

)//)(1()//( LebebLeebebi RRriRRiriv

b

ii i

vR )//)(1( Lebe RRr

)//(////)]//)(1([// LebbLebebii RRRRRRrRRR

Let’s find Ri :

Page 24: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Common-Collector Amplifier

Ro

(b)

I

IRe

Let’s find Ro :

bb IIII Re

)1()//(11

1

bsbee

o

RRrRivR

Re eI I I Re eI I I

1Re e Re bI I I I I

bsbee RRrv

Rv

//)1(

1

)//(// bsbee

RRrR

IeI

ReI

Page 25: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Common-Collector Amplifier

Ro

(b)

I

IRe

Ri (a)

bLebei RRRrR //)]//)(1([

1)//(

// bsbeeo

RRrRR

Page 26: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsSingle-Stage BJT Amplifiers

Common-Collector Amplifier

bLebei RRRrR //)]//)(1([

1

)//(// bsbe

eoRRr

RR

C-C amp characteristics:• Voltage gain is less than unity, but close (to unity) since β is large and rbe is small.• Also called an emitter follower since the emitter follows the input signal.• Input resistance is higher, output resistance is lower. - Used for connecting a source with a large Rs to a load with low resistance.

(a) 共集电极电路

1)//)(1(

)//(

Lebe

Le

i

OV RRr

RR

V

VA

iAL

Le

RRR )//)(1(

>>1

Page 27: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Single-Stage BJT AmplifiersCommon-Base Amplifier

(a) 共基极电路

Rc

2b2b1b

CCB R

RRVV

eEBEB RIVV e

B

e

BEBEC R

VR

VVII

C

BI

I )( eCCCCeECCCCCE RRIVRIRIVV

Ground the base and drive the input signal into the emitter

Page 28: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Single-Stage BJT AmplifiersCommon-Base Amplifier

(a) 共基极电路 Ri

Ro

be

Lc

beb

Lccv r

RRri

RRiA

)//()//(

i

oi I

IA

1

)1()(

//)1(

)(

C

ELC

C

ebe

be

LC

C

IIRR

R

Rrr

RRR

For RL<<RC, CEi IIA

since1)1(

e

be Rr

//)1(

Ri=

Ro≈RC

Page 29: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Single-Stage BJT AmplifiersCommon-Base Amplifier

(a) 共基极电路

be

Lcv r

RRA )//(

i

oi I

IA

LC

CLC

C

RRRRR

R

)1(

)(

For RL<<RC, 1)1(

iA

)1(//

)1(

be

ebe rRr

Ri=

Ro≈R

C CB amp characteristics:• current gain has little dependence on β• is non-inverting• most commonly used as a unity-gain current amplifier or current buffer and not as a voltage amplifier: accepts an input signal current with low input resistance and delivers a nearly equal current with high output impedance• most significant advantage is its excellent frequency response

Page 30: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

C-C C-E C-B

Input

Output

Functions

Summary for three types of diodes:

BI BIBI

EI CI CI

Basic BJT Amplifiers Circuits

Zout < ZinVout > Vin

Zout > ZinVout > VinVout ≈ Vin

Zout > Zin

Page 31: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Frequency Response

Key Words: Basic Concepts High-Frequency BJT Model Frequency Response of the CE Amplifier

Page 32: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Frequency ResponseBasic Concepts

Time

0.5ms 1.0ms 1.5ms 2.0ms 2.5ms 3.0ms 3.5ms 4.0msV(1) V(2)

-1.0V

-0.5V

0V

0.5V

1.0V

Page 33: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Frequency ResponseBasic Concepts

Frequency0Hz 2KHz 4KHz 6KHz 8KHz 10KHz 12KHz 14KHz 16KHz 18KHz 20KHzV(2) V(1)

0V

200mV

400mV

600mV

800mV

Frequency

10Hz 100Hz 1.0KHz 10KHz 100KHz 1.0MHzV(2)

0V

0.5V

1.0V

Page 34: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsFrequency Response

Basic Concepts

Lower cut off frequency Upper cut off frequency

)()()()( vvv AAorffAA

The drops of voltage gain (output/input) is mainly due to:1 、 Increasing reactance of (at low f)2 、 Parasitic capacitive elements of the network (at high f)3 、 Dissappearance of changing current (for transformer coupled amp.)

ecs CCC ,,

Page 35: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

Frequency Response

C

C

In BJTs, the PN junctions (EBJ and CBJ) also have capacitances associated with them

rbe

C

C

C'rbe C'

High-Frequency BJT Model

Page 36: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

vs

Frequency ResponseFrequency Response of the CE Amplifier

C'rbe C'

There are three capacitors in the circuit.

At the mid frequency band, these are considered to be short circuits and internal capacitors and are considered to be open circuits.

C',C'

Page 37: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

vs

Frequency ResponseFrequency Response of the CE Amplifier

At low frequencies, C1, C2 are an open circuit and the gain is zero. Thus C1 has a high pass effect on thegain, i.e. it affects the lower cutoff frequency of the amplifier.

)////( 2111 bebbs rRRRC

2 is the time constant for C2. 12 ---is neglected

11 2

1

Lf

Page 38: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers Circuits

vs

Frequency ResponseFrequency Response of the CE Amplifier

)////( 2111 bebbs rRRRC

12 ---is neglected

Capacitor Ce is an open circuit. The pole time constant is given by the resistance multiplied by Ce.

eebesb

e CRrRR

//1

)//(

222

211.1 LeLLL ffff

eLef

21

Page 39: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

C'rbe C'

Basic BJT Amplifiers CircuitsFrequency Response

Frequency Response of the CE Amplifier

vs

At high frequencies, C1, C2 Ce are all short circuit. The frequency that dominates is thelowest pole frequency.

The time constant is neglected for)1( '

CjRL C'

CrRR besbC )////(

C

Hf

2

1

In summary:the lower cut off frequency is determined by network capacitence. e.g. The higher cut off frequency is determined by the parasitic ferquency of the BJT. e.g.

C

eCCC ,21

Page 40: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

C'rbe C'

Basic BJT Amplifiers CircuitsFrequency Response

Frequency Response of the CE Amplifier

vs )1)(1(HL

Lvmv

ffj

ffj

ffj

AA

frequency-mid0,, —vmv

HLHL AA

ff

fffffFor

frequency-low1

,0),( —

L

Lvmv

HHL

ffj

ffj

AAffffffFor

frequencyHigh

ffj

AAffffffFor

H

vmvL

LH

—1

1,0)(

Page 41: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsFrequency Response

vs

)1)(1(HL

Lvmv

ffj

ffj

ffj

AA

H

HH

L

LL ff

21

221

2

C'rbe C'

Frequency Response of the CE Amplifier

Page 42: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

Basic BJT Amplifiers CircuitsFrequency Response

decadedecade

0

Frequency Response of the CE Amplifier

Page 43: Lecture no 2 to 5 THE BASIC BJT AMPLIFIER CONFIGURATIONS

For student References.

Chapter 9 amplifier fundamentals (9.1) (9.2) from the book Electronic devices, circuit and systems (Micheal M cirovic)

Chapter 8 introduction to amplifiers (8.1) (8.2) from the book introductory electronic devices and circuits by author (Robert T .paynter).

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