chapter 5 - ele232_feb11 [compatibility mode]
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ac bjt analysisTRANSCRIPT
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Chapter 5 : AC Analysis of BJT
Norsabrina SihabFaculty of Electrical Engineering,Universiti Teknologi MARAPulau PinangTel : 04-3823355Email : [email protected]
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Chapter 5 – AC Analysis of BJT
Learning Outcome
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Learning Outcome
At the end of this chapter, students able to:Analyze the small signal of single stage BJT amplifier circuitsCalculates the transistor parameters such as voltage gain Av, Ca cu ates t e t a s sto pa a ete s suc as o tage ga v,current gain Ai, input impedance Zi and output impedance Zo.
Electronics 1 Updated May 2011Norsabrina Sihab
Chapter 5 – AC Analysis of BJT3
IntroductionIntroduction
Increasing the power of an AC signal is called amplification.I th l l k it k i l bIncrease the power level - make it a weak signal become more stronger.Amplification circuit called amplifier eg. Bipolar transistorAmplifie p ope tiesAmplifier properties:
1. Voltage gain, AV
2. Current gain, Ai
3 I t i d Z3. Input impedance, Zi
4. Output impedance, Zo
Good Amplifier:h l1. High Voltage gain, AV
2. High Input impedance, Zi
3. Low Output impedance, Zo
Electronics 1 Updated May 2011Norsabrina Sihab
4. High Bandwidth, BW
Chapter 5 – AC Analysis of BJT4
IntroductionIntroduction
In this chapter we learn how to analyze and work with a single lifistage amplifier.
To examine ac response of BJT Amplifiers by reviewing models frequently used to represent the transistor in ac domain.A lit d f th i t i l ill d t i h th tAmplitude of the input signal will determine whether to use small signal or large signal analysis techniques.
Electronics 1 Updated May 2011Norsabrina Sihab
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Chapter 5 – AC Analysis of BJT5
Transistor Equivalent Model
• A model is an equivalent circuit that represents the AC characteristics of the transistor.A model uses circuit elements that approximate the behavior of• A model uses circuit elements that approximate the behavior of the transistor.
• There are two models commonly used in small signal AC analysis of a transistor:of a transistor:
1. Hybrid -π equivalent model (will be more emphasized)2. re-model
Electronics 1 Updated May 2011Norsabrina Sihab
Chapter 5 – AC Analysis of BJT6
1. Hybrid-π Model only this model being use in ELE232
The hybrid π model is most useful for analysis of high f t i t li tifrequency transistor applications.
At lower frequencies the hybrid π model closely approximate the re parameters, and can be replaced by ethem.
bivg = β
e
bm
mVrr
ivg
261+= )(ββ
π
π
Ee I
r =
Electronics 1 Updated May 2011Norsabrina Sihab
Chapter 5 – AC Analysis of BJT7
2 d l2. re model
BJT b i ll t t ll d d i th f th d lBJTs are basically current-controlled devices, therefore the re-model uses a diode and a current source to duplicate the behavior of the transistor.
One disadvantage to this model is its sensitivity to the DC level ThisOne disadvantage to this model is its sensitivity to the DC level. This model is designed for specific circuit conditions.
The use of re model then becomes more desirable because an important parameter of the equivalent circuit is determined by theimportant parameter of the equivalent circuit is determined by the actual operating conditions but one must still turn to the data sheets for some of the other parameters of the equivalent circuit.
The re model also failed to include the feedback term, which in some e ,cases can be important.
The re model is really a reduced version of the hybrid-π model used extensively for high-frequency analysis.
Electronics 1 Updated May 2011Norsabrina Sihab
Chapter 5 – AC Analysis of BJT8
2. re Transistor Model2. re Transistor Model
b cib
βre
e
βib rce=ro
+
Vbe
_e
Transistor ac equivalent circuit for common emitter
re
e
ie
c
rce=ro
+
Vbe
ie
b_
Transistor ac equivalent circuit for common base
Electronics 1 Updated May 2011Norsabrina Sihab
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Chapter 5 – AC Analysis of BJT9
1a) Common Emitter - by passed RE1a) Common Emitter by passed RE
1. Replace all capacitors with short circuit and set dc source to zero.
1R cR
ccVcircuit and set dc source to zero.
R2R1 Rc
iCoC
Simplified AC equivalent circuit
2R EReC
inv ov
rbb’
b cib
2. Substitute BJT with hybrid-π model.
rπ
e
gmvπ rce
+
Vπ
_
By passed RE
Electronics 1 Updated May 2011Norsabrina Sihab
e
Hybrid-π transistor model
Chapter 5 – AC Analysis of BJT10
Common Emitter - by passed RE
3. Determine the BJT model parameters : Zi Z A and Ai
rbb’b c
+
ib
parameters : Zi, Zo, Av, and Airπ
e
gmvπ rce
+
Vπ
_
R1//R2 Rc
Simplified hybrid-π equivalent circuit of a CE amplifier.
Zi ZoZb
Input impedance
Amplifier with the hybrid-πequivalent circuit
bbbbbb
b
b
rrrriV )1()(Zwhere
Z||R||RZ
''
21i
++=+
==
=
βπ
Electronics 1 Updated May 2011Norsabrina Sihab
ebbbb
b rrii
)1( Zwhere ' ++ β
Chapter 5 – AC Analysis of BJT11
Common Emitter - by passed RE
Output impedance:Voltage gain:
S t Vi t
b
bb
rrandiwhererr
)1(Vg)(i
)r||(RVgVVA
'b
ceCm
i
ov
+==+
−==
ββπ
πSet Vi to zero. Therefore Vπ=0. gmVπ=0 also.
C+
Io
ebbb
b
eb
rrii
rrandiwhere
)r||(R))1((
)r||(RA
)1(Vg
'
ceCv
m
++−
=∴
+
ββ
βββ ππ
rce Rc
+
Vo
-
ebb rr )1()r||(R
'
ceC
++−
=β
β
cer||RZ Co == o
IV
Zo
oI
ivi Z
ZAA =
Current gain without RL:
//RZiZ
vAiA =
Current gain with RL:
Electronics 1 Updated May 2011Norsabrina Sihab
oZ L//RoZ
Chapter 5 – AC Analysis of BJT12
Exercise 1
For the circuit in figure below obtain the + 20Vthe i. Emitter current, IE and reii. Input impedance, Zi, and the
output impedance, Zoiii V lt i A d th t F10
F10μ82k 2k7
iii. Voltage gain, Av and the current gain, Ai
Given that the parameters of the ov
F10μ
1rT
120R33k
transistor is as follows. β=100, rbb’=10Ω, rce=∞Ω and VBE=0.7V. State any assumptions made.
inv
ov
F47μ
18k
120R
1k5
Answer : IE=1.79mA, re=14.53Ω, Zi=1.343kΩ, Zo=2.7kΩ, Av= -168.92, Ai= -90.75
Zi Zo
Electronics 1 Updated May 2011Norsabrina Sihab
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Chapter 5 – AC Analysis of BJT
Exercise
13
A basic common emitter BJT amplifier in below has a quiescent point of the collector current, ICQ = 2 mA. Answer
Exercise
the following :i.Draw the ac equivalent circuitii.Input impendance, Zi
Answer : 478.9Ωiii.Output impedance, Zo
Answer : 2.107kΩiv.Voltage gain, AV
Answer : -151.1v Current Gain A Answer : 34 35v.Current Gain, Ai
Answer : -34.35Use VT = 26mV, Ω=Ω== 100,50,120 bbrkcerβ
+20V
Vo
2.2 k671 IC
C CVi
1.54 k CE
Ci Co
Electronics 1 Updated May 2011Norsabrina Sihab
1.54 k
Zi
Zo
Chapter 5 – AC Analysis of BJT14
1b) Common Emitter – un-bypassed RE1b) Common Emitter un bypassed RE
ccV
1R cR
C C
ovinv
1rT
R
iC oC
R
Ac equivalent circuit
invov2R
eC
LR
Electronics 1 Updated May 2011Norsabrina Sihab
Hybrid-π equivalent circuit of the Common Emitter Amplifier.
Chapter 5 – AC Analysis of BJT15
Common Emitter – un-bypassed RECommon Emitter un bypassed RE
( )//// LRRrvgVVoltage gainInput impedance
( )
( ))1(Vmg
)1)1('(////
errandbiwhereERrbbrbiLRcRcervmg
iVoV
vA
+==+++
−==
βπβπ
βππ
E1' ))((////
iRrri
iVZ
ZRRZ
b
bbb
b
bb
bin
121
+++==
=
βπ
( )
( )////)1)1('(
////
LRcRcerERrbbrbi
LRcRcerbivA
−+++
−=
ββπ
βE1' )( Rrrbb 1+++= βπ
Output impedance ( )1)1(' ERrbbr
Lcce+++
=βπ
Output impedanceSet Vi to zero. Therefore Vπ=0. gmVπ=0 also.
cceo
oo Rr
ivz //==
//RZiZ
vAiA =
Current gain:
Electronics 1 Updated May 2011Norsabrina Sihab
oL//RoZ
Chapter 5 – AC Analysis of BJT16
Exercise 2
For the circuit below, obtain the +20V
i. Emitter current, IE and re
ii. Input impedance, Zi, and the output impedance, Zo
iii Voltage gain A and the current
F10μ82k2k7
iii. Voltage gain, Av and the current gain, Ai
Given that the parameters of the
F10μ
1rT
120R 33kGiven that the parameters of the transistor is as follows. β=100, rbb’=10Ω, rce=∞Ω and VBE=0.7V. State any assumptions made
invov
F47μ
18k120R
1k5
33k
State any assumptions made.
Answer : IE=1.79mA, re=14.53Ω, Zi= 7.08 kΩ, Zo=2.7kΩ, Zi Zo
Electronics 1 Updated May 2011Norsabrina Sihab
Av= -18.35 , Ai= -52.04
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Chapter 5 – AC Analysis of BJT17
Exercise 3
For the circuit below obtain the voltage gain, Av, the current gain, Ai, the input impedance Z and the output impedance Z given that theinput impedance, Zi, and the output impedance, Zo, given that the parameters of the transistor is as follows. β=100, rbb’=75Ω, rce=30kΩ and VBE=0.7V. State any assumptions made.
Answer : re=10.28Ω, Av= -14.136, Zin=8.362kΩ, Zout=2.724kΩ, Ai= -43.346V20V20
3k3k82F10μ
R180k33
F10μ
1rT
invov
k18
R180
R820F47
Electronics 1 Updated May 2011Norsabrina Sihab
F47μ
Chapter 5 – AC Analysis of BJT18
2) Common Base Amplifier2) Common Base Amplifier
rce
cegmvπ+
Vπ
_RE
Rcrπ
e cieib
b
Ac equivalent circuit of a common
rbb’
b’E
Ac equivalent circuit of a common base amplifier.
Hybrid-π equivalent circuit of the Common Base Amplifier
bZi ZoZe
the Common Base Amplifier.
Electronics 1 Updated May 2011Norsabrina Sihab
Chapter 5 – AC Analysis of BJT19
Common Base AmplifierCommon Base Amplifier
Input Impedance Output impedance
)()(//
'' +=
+==
=
ππ bbbbbi
eEi
rrrriVZ
ZRZSet Vi to zero. Therefore Vπ=0. gmVπ=0 also.
Voltage gain
)()( 11 +=
+==
ββbee ii
Z
Voltage gain
cceo
o Rrivz //==
( ))(
//
' π
π
rriRrvg
VVA
bbb
ccem
i
ov +
==
1≈= iZAA
Current gain, Ai
oi
( ) ( ))(
//)(
//)1(
''
ππ
ββββ
rrRr
rriRcriA
rrandiwhere
bb
cce
bbb
cebv
eb
+=
+=
+==Vgm
Electronics 1 Updated May 2011Norsabrina Sihab
1≈=Lo
vi //RZAA)()( '' ππ rrrri bbbbb ++
Chapter 5 – AC Analysis of BJT20
Exercise 4Exercise 4
For the circuit below, obtain the Voltage gain, Av, the input impedance, Ziand the output impedance Z given that the parameter of the transistor isand the output impedance, Zo, given that the parameter of the transistor is as follows. β=100,rb’b=10Ω,rce=∞ and VBE=0.7V. State any assumptions made.
Answer : re=10.28Ω, Av=257.14, Zin=10.27Ω, Zout=2.7kΩ, Ai=0.98
. F10μ
F100μ
F47μ
A common base Amplifier
Electronics 1 Updated May 2011Norsabrina Sihab
A common base Amplifier.
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Chapter 5 – AC Analysis of BJT21
3) Common Collector Amplifier3) Common Collector Amplifier
RER1 R2
ac equivalent circuit of a CC amplifier.
Electronics 1 Updated May 2011Norsabrina Sihab
Hybrid-π equivalent circuit of a CC amplifier.
Chapter 5 – AC Analysis of BJT22
Common Collector AmplifierCommon Collector Amplifier
Voltage gainInput Impedance
ERbiVgbbrrbiiVerrandbiwhere
bZRRiZ
)()'()1(Vmg
//2//1
++++==
=βπβπ EReirbbrbi
ERei
iVoV
vA)'( ++
==π
iERbibibbrerbi
biERbiVmgbbrrbi
biiV
bZ
)()')1((
)()'(
++++=
+++==
ββ
ππ
ERERbirbbrbi
ERbi
)1()1()'(
)1(
+=
++++
=
ββπ
β
biERbbrerbi
bi))1(')1(( ++++
=ββ
ERrbbr )1()'( +++ βπ
ERbbrer )1(')1( ++++= ββ
Electronics 1 Updated May 2011Norsabrina Sihab
Chapter 5 – AC Analysis of BJT23
Common Collector Amplifier
Vi=0
rbb’ rπb e
gmvπ RE
+ Vπ -
ib ie
R1//R2
+
Vo
Output impedanceSet Vi to zero.
rbb’ rπ eib i
c--
π−+−
==
=)'('
'//
eibbrrbi
xixV
oZ
oZERoZ
rbb rπ e
gmvπ RE
+ Vπ -
ib ie
+
Vo
βπ
ππ
++
=
++
=
)'(
)'(
bibibbrrbiVmgbibbrrbi
Zo=RE//Zo’c
--
rbb’ rπ eib ieZo’β
π
β
++
=
+
1'bbrrbibi
e
gmvπ
+ Vπ -
b e
VX
ix
zCurrent gain
Electronics 1 Updated May 2011Norsabrina Sihab
Zo’c
LRzzAA
o
ivi //
=
Chapter 5 – AC Analysis of BJT24
Exercise 5Exercise 5
For the circuit in figure below obtain the V20the i. Emitter current, IE and re
ii. Input impedance, Zi, and the output impedance, Zo
7k2k82p p , o
iii. Voltage gain, Av and the current gain, Ai
iC
Given that the parameters of the transistor is as follows. β=100, rbb’=10Ω, rce=∞Ω and VBE=0.7V.
invovk18 0k1
bb ce BE
State any assumptions made.
Answer : IE=2.53mA, re=10.28Ω, Zi=12.89kΩ, Zo=10.27Ω, Av= 0.99, Ai= 1.24k
Common collector Amplifier circuit.
Electronics 1 Updated May 2011Norsabrina Sihab
i o v i
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Chapter 5 – AC Analysis of BJT25
TutorialTutorial
1. Determine Zin, Zo, AV and AVS β=150 r =10Ω r =50kΩβ=150,rb’b=10Ω,rce=50kΩand VBE=0.7V. State any assumptions made.
Electronics 1 Updated May 2011Norsabrina Sihab
Chapter 5 – AC Analysis of BJT26
TutorialTutorial
2. Determine Zin, Zo, AV, Ai, and AVS. Vo when V 25 V β 120 10Ω Ω d V 0 7VVs=25mV. β=120,rb’b=10Ω,rce=∞Ω and VBE=0.7V. State any assumptions made.
A I 7 81 A 3 33Ω Z 412 2Ω Z 1 8kΩ A
Vcc = +24V
Answer: IE=7.81mA, re= 3.33Ω, Zin = 412.2Ω , Zo = 1.8kΩ, AV= -338.27, Ai = -119.79, and AVS =-137.75. Vo = 3.45V
Ci
Co
R1240k
RC1k8
Vo
VRS
600R
RE1k0
Vi
CE
VS
600Rβ=120
RL3k3
Electronics 1 Updated May 2011Norsabrina Sihab
Zi Zo