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8/14/2019 Chapter 1 BJT Amplifier
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Bipolar Junction Transistor (BJT)
and Linear Amplifier
Chapter 1BJT Amplifiers
1 2013/2014 EKT204
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Outline
2013/2014 EKT2042
IntroductionBJT Linear AmplifierGraphical Analysis & AC Equivalent CircuitSmall-signal hybrid- equivalent circuit
Hybrid- Equivalent Circuit and Early EffectExpanded Hybrid- Equivalent CircuitAC Load Line AnalysisMaximum Symmetrical Swing Common-emitter AmplifierCommon-collector AmplifierCommon-base Amplifier
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Introduction
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Analog Electronic Circuits Analog Electronic Circuits produce ananalog signals
Linear amplifier circuitMagnifies input signal & produce output
signal that is larger & directlyproportional to input signalElectronic
CircuitSignalInput
SignalOutput
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BJT Linear AmplifierBJT needs to be biased with DC voltage atquiescent point (Q-point) where BJT is biased inforward active region
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Linear Amplifier
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Time-varying output voltage is directlyproportional to & larger than time-varying inputvoltage
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Graphical Analysis & ACEquivalent Circuit
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A common -emitter circuit with time-varyingsignal source in series with the base DC source
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Graph plots collector current (i c) vs collector-emitter potential (v CE ).For different base currents (i B) different curves are obtained.
AC base current superimposed on I BQ - time-varying base current inducesac collector current superimposed on I CQ
AC collector-emitter voltage = output voltage - is larger than the input =amplificationLinear amplifier = ac added / superimposed on dc ==> superposition ==>only if ac is small ==>small signal analysis .
Line between VCC /R C and V CC = dc load line
Q-point is chosen wheredistance between i B curves aresimilar / even so thatamplification properties arelinear.
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Contd time-varying signals linearly related & superimposedon dc values)
If signal source, v s = 0:
(4)
(3) (2)
(1)
be BEQ BE
ceCEQCE
cCQC
b BQ B
vV v
vV vi I i
i I i
(6) loop)E-(C
(5) loop)E-(B
CEQC CQCC
BEQ B BQ BB
V R I V
V R I V
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Contd For B-E loop, considering time varying signals:
Rearrange:
Base on (5), left side of (7) is 0. So:
For C-E loop, considering time varying signals:
9Base on (6), left side of (11) is 0. So:
(7) )()( be BEQ Bb BQ BE B B s BB vV Ri I v RivV
(8) sbe Bb BEQ B BQ BB vv RiV R I V
(9) be Bb s v Riv
(11) (10)
ceccCEQC CQCC
ceCEQC cCQCE C C CC
v RiV R I V vV Ri I v RiV )()(
(12) 0 cecc v Ri9 2013/2014 EKT204
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I B versus V BE Characteristic
b BT
be BQ B i I V
v I i )1(
Time-varying signal source, v s appliedto base - time-varying base currentcomponent
==> there is a time-varying base-emitter component
Figure shows exponential relationship
between i B vs v BE
IF MAGNITUDES of time-varyingsignals superimposed on dc Q-pt aresmall => develop linear relationshipbetween ac v BE and ac i B
This relationship corresponds to slopeof curve at the Q-pt.
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Rules for AC Analysis
Replacing all capacitors by short circuits
Replacing all inductors by open circuits
Replacing dc voltage sources by ground connections
Replacing dc current sources by open circuits
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AC Equivalent Circuitfor Common Emitter
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EquationsInput loop
Output loop
beT
BQb
be Bb s
vV
I i
v Riv
bc
ceC c
ii
v Ri
00.026 V
The DC voltage sources have been set equal to zero or ground(V CC =0).Only ACc condition are to be considered.
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Small Signal AC Equivalent Circuit
ac input signal voltages and currents are in the orderof 10 percent of Q-point voltages and currents.
e.g. If dc current is 10 mA, the ac current (peak-to- peak) < 0.1 mA.
13 2013/2014 EKT204
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Small-signal hybrid- equivalent circuit
BQ F CQ
CQ
T F
BQ
T
b
be
I I
I V
I V
r iv
,
g m =I CQ /V T
r = VT/I CQ
v be = i b r
r = diffusion
resistance /base-emitter inputresistance
1/r = slope of i B
V BE curve
14
Phasor signals are shown in parentheses.
r g mCommon-Emitter Current Gain, as constant;2013/2014 EKT204
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)( b
b
I
i
Using common-emitter current gain ( ) parameter
Small-signal hybrid- equivalent circuit
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How to construct Small-signal hybrid-
Place a terminal for the transistor
Common Terminal as ground
B
E
C
We know that
i across B ib
i across C i b
i across E (+1)i b
r between B -E
R C
R B
v s
v O
V BB
V CC
B
E
C
ibr
16 2013/2014 EKT204
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C bemceo RV g V V s B
be V Rr r
V
BC m
s
ov Rr
r R g
V V
A
gain,voltagesignalSmall
Output signal voltage
Input signal voltage17
Small-signal Voltage Gain
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Problem-Solving Technique:BJT AC Analysis
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1. Analyze circuit with only dc sources to find Qpoint.
2. Replace each element in circuit with small-signal model, including the hybrid model forthe transistor.
3. Analyze the small-signal equivalent circuitafter setting dc source components to zero.
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Transformation of Elements
Element DC Model AC Model
Resistor R R
Capacitor Open C
Inductor Short L
Diode +V g, r f r d = V T /I D
Independent Constant
Voltage Source
+ V S - Short
Independent ConstantCurrent Source
IS Open
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Example 1
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Determine the small signalvoltage gain, including theeffect of the transistoroutput resistance, r o.
Assume the transistor &circuit parameter are =100,VCC=12V, V BE=0.7V,RC=6k, RB=50k andVBB=1.2V.
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21
Solution 1Do the dc analysis to find Q-point values
Determine the small signal output resistance ,
Do the ac analysis to find the small signal base-emitter input resistance,r , transconductance, g m and then voltage gain, AV
V k m R I V V
mA I I
A RV V
I
C CQCC CEQ
BQCQ
B
BE BB BQ
6)6)(1(12 then,
1)10(100thatso
10507.02.1
k m I
V r
CQ
Ao 50
1
50
4.11506.2
6.2)6(5.38)(
/5.38026.0
1
6.21
)026.0(100
m
Rr r
R g V V
A
V mAm
V
I g
k m I
V r
BC m
S
oV
T
CQm
CQ
T
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Hybrid- Equivalent Circuitand Early Effect
transconductanceparameter
current gainparameter
r o =V A/I CQ
r o = small-signaltransistor output
resistance V A = early voltage22 2013/2014 EKT204
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Early Voltage(V A )
Early Effect
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Example 2 If the Early voltage, V A is 50 V, reconsider thecircuit in example 1 and determine the small-signal voltage gain including the effect of thetransistor output resistance, r 0 .
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Solution 3
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C omo Rr V g V
r R R Ri 21 C oo Rr R
sS
V Rr R R
r R RV
21
21
C oS
m s
ov Rr Rr R R
r R R g
V V
A
21
21
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Expanded Hybrid- EquivalentCircuit
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h-Parameter Model for npn
fe
bie
h
r r r h
ooe
re
r r h
r
r h
11
29 2013/2014 EKT204
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T-Model of an npn BJT
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4 Equivalent 2-port Networks
Voltage Amplifier
Current Amplifier
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Cont
Transconductance Amplifier
Transresistance Amplifier
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Small Signal Equivalent Circuit
If
The coupling capacitor is assumed to be a shortcircuit. (If signal source >>> 2kHz)
TH cC R
fC Z
2
1
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2013/2014 EKT20436
ExampleDetermine the small voltage gain for the circuit below if=100, VCC=5V, V BE=0.7Vand V A=100V
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2013/2014 EKT204 37
SolutionDo the dc analysis to find Q-point values
V k m R I V V mA I I
Ak R
V V I
V V R R R
V
k k
k k R R
R R R
C CQCC CEQ
BQCQ
TH
BE TH BQ
CC TH
TH
31.6)6)(95.0(12 then,95.0)5.9(100thatso
5.99.5
7.0756.0
756.0)12(1003.6
9.5100
)3.6)(7.93(
21
2
21
21
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2013/2014 EKT20438
SolutionDetermine the small signal output resistance ,
Do the ac analysis to find the small signal base-emitter input resistance,r , transconductance, g m and then voltage gain, AV
k m I V
r CQ
Ao 3.10595.0100
1635.087.1
87.1)3.105//6(5.36
////
)//(
/5.36026.095.0
74.295.0
)026.0(100
k m
R Rr Rr
r R g V V
A
V mAm
V
I g
k m I
V r
S TH
TH oC m
S
oV
T
CQm
CQ
T
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The basic common-emitter circuit used inprevious analysis causes a serious defect :
If BJT with V BE =0.7 V is used, I B=9.5 A & I C=0.95 mA
But, if new BJT with V BE =0.6 V is used, I B=26 A & BJTgoes into saturation; which is not acceptable Previouscircuit is not practicalSo, the emitter resistor is included: Q-point is stabilizedagainst variations in , as will the voltage gain, A V
AssumptionsCC acts as a short circuitEarly voltage = ==> r o neglected due to open circuit
Basic Common-Emitter Amplifier
39
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2013/2014 EKT20440
Circuit with Emitter ResistorTo improve dc biasing designAV with R E less dependent on.VA infinite, r o open circuit.
C bo R I V )(tage,output volac
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Common-Emitter Amplifierwith Emitter Resistor
ac output voltage
Input voltage loop
Input resistance, R ib
Input resistance to amplifier, Ri
Voltage divider equation of V in to V s
Remember : Assume VA is infinite , r o is neglected
C bo R I V
E bbbin R I I r I V
E b
inib Rr I
V R 1
ibi R R R R 21
s
S i
iin V
R R
RV
41
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2013/2014 EKT20442
E
C
E
C V
E si
si
i
E
C
ib
in
s
C
s
C b
s
oV
s si
iin
ibi
E
b
inib
E bbbin
R R
R R
A
r R R R
R R R
Rr R
RV
V R
V R I
V V
A
V R R
RV
R R R R
Rr I
V R
R I I r I V
)1(
)1( and if
)1()(
////,resistanceinput
effectrulereflectionresistance)1(
)(
21
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2013/2014 EKT20443
Example
Determine the small voltage gain for the circuitwith an emitter resistor below if =100,VBE=0.7Vand V A=.
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2013/2014 EKT20444
Solution
0.5
)1( and if
53.4
06.8////
6.41)1(
/1.83
2.1
81.4;16.2
21
V
E si
s
oV
ibi
E b
inib
CQ
A
o
T
CQm
CQ
T
CEQCQ
A
r R R R
V V A
k R R R R
k Rr I V
R
I V
r
V mAV
I g
k I V
r
V V mA I
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2013/2014 EKT20445
Circuit with Emitter BypassCapacitor
Use to effectively to short out a portion @ all of emitterresistance by the ac signal .
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R S
R 1
R 2 R E
R C
vs
vO
C C
V CC
C E
B C
E
V o
V s R C
RS
r r oR 1||R 2
g m V
Emitter bypass capacitor, C E provides a s h o r t c i r c u i t toground for the ac signals
Common-Emitter Amplifierwith Emitter Bypass Capacitor
Small-signal hybrid-
equivalent circuit
Emitter bypass capacitor isused to short out a portion orall of emitter resistance bythe ac signal. Hence no REappear in the hybrid- equivalent circuit
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Common-emitter Amplifier withEmitter Bypass Capacitor
47
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AC Load Line - KVL on C-E loop
1
11
1
1- Slope
)(
Assuming
0
E C
E C c E cC cce
ec
E eceC c
R R
R Ri Ri Riv
ii
Riv Ri
49
Visualized the relationshipbetween small-signalresponse & transistorcharacteristics
Occurs when capacitorsadded in transistor circuit
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50
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Example (DC & AC Load Line)
Determine the dc and ac load line. V BE=0.7V, =150, VA=
51
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Solution
To determine dc Q-point, KVL around B-E loop
k R R-
R I R I V V V
mA I I mA I I
A R R
V V I
R I V R I R I V R I V
E C
E EQC CQCEQ
BQ EQ BQCQ
E B
EB BQ
E BQ EB B BQ E E EB B BQ
1511 Slope
53.6)( point,-QFor
9.0)1( & 894.0Then
96.5)1(
)1(
52
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)//()//)((
/4.34
36.4
53.6;894.0
LC c LC meo
CQ
Ao
T
CQm
CQ
T
ECQCQ
R Ri R Rv g vv
I V
r
V mAV
I g
k I
V r
V V mA I
53
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Maximum Symmetrical Swing
When symmetrical sinusoidal signal applied to theinput of an amplifier, the output generated is alsoa symmetrical sinusoidal signal
AC load line is used to determine maximumoutput symmetrical swing
If output is out of limit, portion of the output signal willbe clipped & signal distortion will occur
55
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Maximum Symmetrical Swing
Steps to design a BJT amplifierWrite DC load line equation (relates of I CQ & V CEQ)Write AC load line equation (relates ic , vce ; vce = - icReq ,Req = effective ac resistance in C-E circuit)Generally, ic = I CQ I C (min), where I C (min) = 0 or someother specified min collector currentGenerally, vce = V CEQ V CE(min), where V CE(min) issome specified min C-E voltageCombination of the above equations produce optimumI CQ & V CEQ values to obtain maximum symmetricalswing in output signal
56
E l (M i S i l S i )
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Example (Maximum Symmetrical Swing )
Determine the maximum output symmetrical swing for the ac loadline in previous figure.
SolutionFrom the dc & ac load line, the maximum negative swing in the I c is from0.894 mA to zero (I CQ). So, the maximum possible peak-to-peak ac
collector current:
The max. symmetrical peak-to-peak output voltage:
Maximum instantaneous collector current:
mA79.1)894.0(2(min))(2 C CQc I I i
V56.2)2||5)(79.1()||(|||||| LC ceqcce R Ri Riv
mA79.1894.0894.0||21
cCQC i I i
57
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C-C Small Signal Voltage Gain
CommonCollector Circuit
Small SignalEquivalent
Circuit
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)//(
)1(
E ooo
bo
Rr I V
I I
si
i
E o
E o
s si
iin
E oib
ibb E obobin
R R R
Rr r Rr
V R R
RV
Rr r R R I Rr r I V r I V
)//)(1()//)(1(
VV
A
gainvoltagesignalSmall
)]//)(1([
)]//)(1([
s
ov
59
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C-C Input & Output Impedance
x
xo I
V R
o E s
o
oo E s x
x
m
s
x
o
x
E
x x
s
m x
s
x
o
x
E
xm x
x s
s
x
o
x
E
xm x
r R R R Rr
R
Rr R R R Rr V I
r g
R R Rr V
r V
RV
V R R Rr
r g I
R R Rr V
r V
RV
V g I
V R R Rr
r V
R R Rr V
r V
RV
V g I
////1
//// therefore,
111////
1
that Note
////////
//// therefore,
////
////
nodeoutputatcurrentsSumming
21
21
2121
21
21
21
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ExampleCalculate
the small signal voltage gain,the input and output resistance.
Assume the transistor & circuit parameter are; =100, VCC=5V,VBE=0.7V, V A=80V and r o=100k.
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C-C Small Signal Current GainCan be determine by using the input resistance & the concept ofcurrent dividers.
)1(
then,R r andR //R R thatassumeIf
////
)1(
Therefore,
////)1()1(
////
Eoib21
21
21
21
21
21
21
i
E o
o
ibi
ei
o E o
oe
iib
bo
iib
b
i
ei
A
Rr r
R R R R R
I I
A
I Rr
r I
I R R R
R R I I
I R R R
R R I
I I A
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Common Base Amplifier
63
C B S ll Sig l E i l t
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C-B Small Signal EquivalentCircuit
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C-B Small Signal Voltage Gain
zero]approachesR [as )//(
////11
)//(
////1
then,
since 111
E]nodeatEquation[KCL 0)(
)//)((
S LC mV
S E S
LC m s
o
V
S E S
s
mS
s
S E
S
s
E m
LC mo
R R g A
R Rr
R R R g V V
A
R Rr
RV
V
r g R
V
R Rr V
RV V
RV
r V
V g R RV g V
65
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C-B Small Signal Current Gain
infinity]approachesREandzeroapproachesR [as 1
1
//1
then,
)(
//1
E]nodeatEquation[KCL 0
L
r g A
Rr
R R R
g I I
A
R R RV g I
Rr
I V
RV
r V V g I
mi
E LC
C m
i
oi
LC
C mo
E i
E mi
66
d
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Input Impedance
ei
ie
mmbi
r r
I V
R
r V V g
r V
V g I I
1
resistanceInput
1
inputat theKCL
67
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Output Impedance
C o
S E m
R R
RV
RV
r V
V g
resistanceoutputThe
0Vgmeans0,VimpliesThis
0
emitter at theKCL
zero.toequalset beenhasv
m
s
68
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Summary & ComparisonConfiguration Common
EmitterCommonCollector
Common Base
Voltage Gain Av > 1 Av 1 Av > 1
Current Gain Ai > 1 Ai > 1 Ai 1
InputResistance
Moderate(k)
High(50-100k)
Low()
OutputResistance
Moderate toHigh
Low Moderate toHigh