ANALOG ELECTRONIC CIRCUITS 1 EKT 204 Basic BJT Amplifiers (Part 2) 1.

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ANALOG ELECTRONIC CIRCUITS 1 EKT 204 Basic BJT Amplifiers (Part 2) 1

Transcript of ANALOG ELECTRONIC CIRCUITS 1 EKT 204 Basic BJT Amplifiers (Part 2) 1.

Page 1: ANALOG ELECTRONIC CIRCUITS 1 EKT 204 Basic BJT Amplifiers (Part 2) 1.

ANALOG ELECTRONIC CIRCUITS 1

EKT 204

Basic BJT Amplifiers (Part 2)

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The basic common-emitter circuit used in previous analysis causes a serious defect : If BJT with VBE=0.7 V is used, IB=9.5 μA & IC=0.95 mA

But, if new BJT with VBE=0.6 V is used, IB=26 μA & BJT goes into saturation; which is not acceptable Previous circuit is not practical

So, the emitter resistor is included: Q-point is stabilized against variations in β, as will the voltage gain, AV

Assumptions CC acts as a short circuit

Early voltage = ∞ ==> ro neglected due to open circuit

Basic Common-Emitter Amplifier

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Common-Emitter Amplifier with Emitter Resistor

CE amplifier with emitter resistor Small-signal equivalent circuit (with current gain parameter, β)

inside transistor

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Common-Emitter Amplifier with Emitter Resistor

ac output voltage

Input voltage loop

Input resistance, Rib

Input resistance to amplifier, Ri

Voltage divider equation of Vin to Vs

Remember: Assume VA is infinite, ro is neglected

Cbo RIV

Ebbbin RIIrIV

Eb

inib Rr

I

VR 1

ibi RRRR 21

sSi

iin V

RR

RV

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Common-Emitter Amplifier with Emitter Resistor

Cont..

So, small-signal voltage gain, AV

If Ri >> Rs and (1 + β)RE >> rπ

Remember: Assume VA is infinite, ro is neglected

Si

i

E

Cv

sib

inC

s

Cb

s

ov

RR

R

Rr

RA

VR

VR

V

RI

V

VA

1

1

E

C

E

Cv R

R

R

RA

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RS

R1

R2 RE

RC

vs

vO

CC

VCC

CE

B C

E

Vo

Vs RC

RS

r roR1|| R2 gmV

Emitter bypass capacitor, CE provides a short circuit

to ground for the ac signals

Common-Emitter Amplifier with Emitter Bypass Capacitor

Small-signal hybrid-π equivalent circuit

Emitter bypass capacitor is used to short out a portion or all of emitter resistance by the ac signal. Hence no RE appear in the hybrid-π equivalent circuit

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DC & AC LOAD LINE ANALYSIS

DC load line Visualized the relationship between Q-point & transistor

characteristics

AC load line Visualized the relationship between small-signal response &

transistor characteristics Occurs when capacitors added in transistor circuit

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Common Emitter Amplifier with emitter bypass capacitor

Common-emitter amplifier with emitter bypass capacitor

Example 1

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DC Load Line

KVL on C-E loop

21

21

21

21

21

1 Slope

)( So,

11

1, when point,-QFor

)(1

1 when ,)(

1

)(

EEC

EECCQCEQ

EECCCCE

CEEECCECC

EEECECC

RRR

-

RRRIVVV

RRIRIVVV

IIVRRIVRI

VRRIVRIV

Solution...

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KVL on C-E loop

AC Load Line

1

11

1 0

EC

ECcEcCcce

ec

EeceCc

RR

RRiRiRiv

ii

RivRi

1- Slope

Assuming

)(

AC equivalent circuit

Solution...

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DC & AC Load Lines

Full solution

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AC LOAD LINE ANALYSISDetermine the dc and ac load line. VBE=0.7V, β=150, VA=∞

Example 2

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DC Load Line

To determine dc Q-point, KVL around B-E loop

kRR

-

RIRIVVV

mAIImAII

ARR

VVI

RIVRIRIVRIV

EC

EEQCCQCEQ

BQEQBQCQ

EB

EBBQ

EBQEBBBQEEEBBBQ

15

11 Slope

53.6)( point,-QFor

9.0)1( & 894.0Then

96.5)1(

)1(

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AC Load Line

)//()//)((

/4.34

36.4

53.6;894.0

LCcLCmeco

CQ

Ao

T

CQm

CQ

T

ECQCQ

RRiRRvgvv

I

Vr

VmAV

Ig

kI

Vr

VVmAI

Small signal hybrid-π equivalent circuit

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DC & AC Load lines

Full solution

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Maximum Symmetrical Swing

When symmetrical sinusoidal signal applied to the input of an amplifier, the output generated is also a symmetrical sinusoidal signal

AC load line is used to determine maximum output symmetrical swing If output is out of limit, portion of the output signal will be

clipped & signal distortion will occur

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Maximum Symmetrical Swing

Steps to design a BJT amplifier for maximum symmetrical swing:

Write DC load line equation (relates of ICQ & VCEQ) Write AC load line equation (relates ic, vce ; vce = - icReq,

Req = effective ac resistance in C-E circuit) Generally, ic = ICQ – IC(min), where IC(min) = 0 or some

other specified min collector current Generally, vce = VCEQ – VCE(min), where VCE(min) is

some specified min C-E voltage Combination of the above equations produce optimum

ICQ & VCEQ values to obtain maximum symmetrical swing in output signal 17

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Maximum Symmetrical SwingExample 3

Determine the maximum symmetrical swing in the output voltage of the circuit given in Example 2.

Solution: From the dc & ac load line, the maximum negative swing

in the Ic is from 0.894 mA to zero (ICQ). So, the maximum possible peak-to-peak ac collector current:

The max. symmetrical peak-to-peak output voltage:

Maximum instantaneous collector current:

mA 79.1)894.0(2(min))(2 CCQc IIi

V 56.2)2||5)(79.1()||(|||||| LCceqcce RRiRiv

mA 79.1894.0894.0||2

1 cCQC iIi 18

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Self-Reading

Textbook: Donald A. Neamen, ‘MICROELECTRONICS Circuit Analysis & Design’,3rd Edition’, McGraw Hill International Edition, 2007

Chapter 6: Basic BJT Amplifiers Page: 397-413, 415-424.

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Exercise

Textbook: Donald A. Neamen, ‘MICROELECTRONICS Circuit Analysis & Design’,3rd Edition’, McGraw Hill International Edition, 2007

Exercise 6.5, 6.6, 6.7,6.9 Exercise 6.10 , 6.11

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