Electronics Lecture10 11Amplifiers · Email: [email protected] . Korea University of Technology...
Transcript of Electronics Lecture10 11Amplifiers · Email: [email protected] . Korea University of Technology...
Korea University of Technology & Education
Department of Electrical, Electronics and Communications Engineering
Department of EECE
BJT Amplifiers
Electronic Circuits
Manar Mohaisen Office: F208
Email: [email protected]
Korea University of Technology & Education
Department of Electrical, Electronics and Communications Engineering
₪ Explain the DC Operating Point
₪ Explain the Voltage-divider Bias
₪ Other Bias Methods
₪ Discussions
Review of the Precedent Lecture
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₪ Explain the Amplifier Operation
₪ Explain the BJT AC Models
₪ The Common-emitter Amplifier
₪ The common-base amplifier
₪ The common-collector amplifier
₪ Multi-stage amplifiers
Class Objectives
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₪ Quantities DC Quantities
Uppercase italic letters
Uppercase subscripts
IB, VC
AC Quantities Uppercase italic letters
Uppercase subscripts
Ib, Ve
Instantaneous Quantities Uppercase italic letters
Uppercase subscripts
ib, vc
Resistances RC DC Resistance, Rc AC resistance, r’e internal ac resitance.
Amplifier Operation
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₪ The Linear Amplifier Coupling capacitors block the DC quantities.
Prevents the change of the DC bias voltages at the base and collector.
Collector voltage is inversely proportional to Ic. It has a 180 phase difference with Ic.
Amplifier Operation – contd.
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₪ Graphical Representation AC load line.
Difference bet. DC and AC load line will be revisited in Chapter 7.
Amplifier Operation – contd.
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₪ Example 6.1
Amplifier Operation – contd.
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₪ r Parameters
r’b (small) can be neglected (short)
r’c (high) can be neglected (open)
Transistor AC Models – contd. r Param. Description
αac ac alpha
βac ac beta
r‘e ac emitter resistance
r‘b ac base resistance
r‘c ac collector resistance
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₪ Determining r’e by a Formula
Note that Emitter current changes with temperature.
Also, in the derivation, it was considered that there is an abrupt junction between the n and p regions.
However, this approximation is valid for analysis.
Transistor AC Models – contd.
' 25mVe
Er I=
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₪ Comparison between the AC Beta and the DC Beta
Transistor AC Models – contd.
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₪ h (hybrid) Parameters Supplied by the manufacturer.
Transistor AC Models – contd.
H Parameter Description Condition
hi Input impedance (resistance) Output shorted
hr Voltage feedback ratio Input open
hf Forward current gain Output shorted
ho Output admittance (conductance) Input open
Configuration Description
Common-emitter hie, hre, hfe, hoe
Common-base hib, hrb, hfb, hob
Common-collector hic, hrc, hfc, hoc
ac fbhα =
ac fehβ =
' reeoe
hr h=
' 1recoe
hr h+=
' (1 )reieb feoe
hr h hh= − +
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₪ Amplifier DC Analysis & AC Analysis
Common-emitter refers to the AC operation.
The Common-emitter Amplifier
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₪ DC Analysis Q-point
> 10 R2, so it is neglected.
The Common-emitter Amplifier – contd.
EDCN(BASE) (150)(560 ) 84 kΩIR Rβ= = Ω =
2B CC
1 2
6.8 k 12V 2.83V28.8kRV VR R
⎛ ⎞ ⎛ ⎞⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎝ ⎠⎝ ⎠
Ω≅ = =+ Ω
E B BEE
E E
2.83V 0.7V 3.80mA560V V VI R R
− −= = = =Ω
C CC C C 8.2VV V I R= − =
ECE C 6.07VV V V= − =
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₪ AC Analysis C1, C2, and C3 are replaced by shorts.
Their values are selected so that their impedances are negligible.
The DC source is replaced with ground.
The Common-emitter Amplifier – contd.
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₪ AC Analysis The ac input resistance is seen in parallel with R1 & R2.
The Common-emitter Amplifier – contd.
1 2( ) ( )|| ||in tot in baseR R R R=
( )
( )
in totsb sin tot
RV VR R
⎛ ⎞⎜ ⎟⎜ ⎟⎜ ⎟⎝ ⎠
= +
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₪ Input Resistance looking in at the Base
₪ Output Resistance looking in at the collector
The Common-emitter Amplifier – contd.
( )
' '/
in bin base
in b
e e ac ee ac
VVR I II r rI ββ
= =
= =
'C C|| coutR R r R= ≅
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₪ Example 6-3 Find Vb.
IE = 3.8 mA.
The Common-emitter Amplifier – contd.
'
E
25mV 25mV 6.583.8mAer I= = = Ω
'( ) 160(6.58 ) 1.05kac ein baseR rβ= = Ω = Ω
1 2( ) ( )|| || 873in tot in baseR R R R= = Ω
( )
( )
873 10mV(rms) 7.44mV(rms)1173in tot
sb s in tot
RV VR R
⎛ ⎞ ⎛ ⎞⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎝ ⎠⎝ ⎠
= = =+
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₪ AC Voltage Gain Ratio between Output Voltage
and Input Voltage.
If you would like to get the
overall amplifier voltage gain
The Common-emitter Amplifier – contd.
' ' 'c ec C C Cve e e e eb
I R I R RVA V I r I r r= = ≅ =
( )'
( )
in totc b c vv s s sb in tot
RVV VA AV V V R R
⎛ ⎞⎛ ⎞⎛ ⎞⎜ ⎟⎜ ⎟⎜ ⎟⎜ ⎟⎜ ⎟⎜ ⎟⎜ ⎟⎜ ⎟ ⎜ ⎟⎝ ⎠⎝ ⎠ ⎝ ⎠
= = = +
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₪ Effect of the Emitter Bypass Capacitor On Voltage Gain To obtain a short circuit by the capacitor C2
₪ Example 6-4 Operation frequency range:
200 Hz ~ 10 kHz
The Common-emitter Amplifier – contd.
2 10E
CRX ≤
25610
EC
RX = = Ω
22
1 14.2μF2 CC fXπ= =
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₪ Voltage Gain without the Bypass Capacitor
₪ Example 6-5 r‘e = 6.58 Ω
Gain without Bypass Capacitor
Gain with Bypass Capacitor
The Common-emitter Amplifier – contd.
C've E
RAr R
=+
C'
E
1000 1.76560 6.58ve
RAr R
= = =++
C'
1000 1526.58ve
RAr
= = =
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₪ Effect of Load on the Voltage Gain In presence of a load
The load is connected in Parallel with RC.
Therefore,
The Common-emitter Amplifier – contd.
C' '
|| Lcve e
R RRAr r
= =
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₪ Effect of Load on the Voltage Gain – contd. Example 6-6
RL = 5 kΩ, r‘e = 6.58 Ω, RC = 1 k Ω
In Presence of Load
Without Load
The Common-emitter Amplifier – contd.
C' '
|| 833 1276.58Lcv
e e
R RRAr r
Ω= = = =Ω
C' '
1000 1526.58cve e
RRAr r
Ω= = = =Ω
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₪ Stability of the Voltage Gain Stability is a measure of how well an amplifier maintains its
design values for a change in temperature and β.
₪ Swamping r‘e Reduce its effect.
Both RE1 and RE2 affect the DC bias
Only RE1 affects the AC voltage gain.
The Common-emitter Amplifier – contd.
1
11
'E
'
E, for 10
cve
c eE
RAr R
R R rR
=+
= >
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₪ The Effect of Swamping on the Amplifier’s Input Resistance
The Common-emitter Amplifier – contd.
'1( ) ( )ac e Ein baseR r Rβ= +
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₪ Current Gain Current gain from base to collector
The overall current Gain
with
₪ Power Gain
with
The Common-emitter Amplifier – contd.
cacb
IIβ =
ci s
IA I=( )
sss in tot
VI R R= +
'p v iA A A= ' cv
s
VA V=
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₪ Example 6-8
The Common-emitter Amplifier – contd.
DC analysis
AC analysis
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₪ Example 6-8 – contd. DC Analysis
> 10 R2, so the amplifier is stiff.
The Common-emitter Amplifier – contd.
DC E1 E2IN(BASE) ( ) 150(940 ) 141kR R Rβ= + = Ω = Ω
2B CC
2 11.75VRV VR R
⎛ ⎞⎜ ⎟⎜ ⎟⎜ ⎟⎝ ⎠
≅ =+
E B BE 1.75 0.7 1.05VV V V= − = − =
EE
1 2
1.05V 1.12mA940E E
VI R R= = =+ Ω
C CC C C 10V (1.12mA)(4.7k ) 4.74VV V I R= − = − Ω =
ECE C 4.74 1.05 3.7 VV V V= − = − =
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₪ Example 6-8 – contd. AC Analysis
The Common-emitter Amplifier – contd.
'
E
25mV 25mV 221.12mAer I= = = Ω
1'
( ) )( 175(492 ) 86.1kEac ein base RR rβ += = Ω = Ω
1 2( ) ( )|| || 7.53 kin tot in baseR R R R= = Ω
( )
( )
600 7530attenuation 1.087530s in tots
b in tot
R RVV R
+ += = = = || 4.27kc LCR R R= = Ω
'119.09c cv
e EE
R RA Rr R= ≅ =
+' 1 9.09 8.451.08
bv vs
VA AV⎛ ⎞ ⎛ ⎞⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎝ ⎠⎝ ⎠
= = =
' (8.45)(10mV) 84.5mVc v sV A V= = =
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₪ Example 6-8 – contd. DC & AC Analysis
The Common-emitter Amplifier – contd.
C( )
C( )
Max 1.414 4.74 (84.5mV)(1.414) 4.86 VMin 1.414 4.74 (84.5mV)(1.414) 4.62 V
cc p
cc p
V V VV V V
= + = + =
= + = − =
C( ) ( ) 119 mVout p c pV V V= − =
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₪ Emitter-follower Amplifier Common-collector amplifier
The Common-collector Amplifier
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₪ Voltage Gain
₪ Note Since the output follows the input in both phase and amplitude,
The amplifier is referred to as “emitter-follower”.
The Common-collector Amplifier – contd.
'
'
( )
( )1
out e eve e ein
ee e
V I RA V I r RR
r R
= =+
=+
≅
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₪ Input Resistance
Therefore,
₪ Output Resistance Without load.
The Common-collector Amplifier – contd.
'( )
''
( )
( ) ( )
e e ein bin base
in b b
ac e eb ac e eb
VV I r RR I I II r R r RI
β β
+= = =
+= = +
1 2( ) ( )|| ||in tot in baseR R R R=
||sout Eac
RR Rβ⎛ ⎞⎜ ⎟⎜ ⎟⎝ ⎠
≅
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₪ Current Gain
₪ Power Gain
The Common-collector Amplifier – contd.
( )/e e
iin in in tot
I IA I V R= =
p v i iA A A A= ≅
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₪ The Darlington Pair
Overall current gain
The Common-collector Amplifier – contd.
1 1 1e ac bI Iβ=
2 2 1 22 1e ac ac acb bI I Iβ β β= =
1 2ac acβ β β=
E1 2in ac acR Rβ β=
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₪ An Application Emitter-follower is used as interface bet. A circuit with high
output resistance and low-resistance load.
₪ Example Consider a common-emitter amplifier with RC = 1 kΩ, RL = 8 Ω
The loss in the voltage gain due to the load is high.
W.o. load
w. load
The solution is by using the Darlington pair.
The Common-collector Amplifier – contd.
C'1000 2005v
e
RAr
= = =
C' '
|| 7.94 1.595Lcv
e e
R RRAr r
= = = =
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₪ An Application Interface the amplifier and the speaker.
The Common-collector Amplifier – contd.
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₪ Example 6-10 Common-emitter:
r‘e = 5 , VCC = 12 V, RC = 1 k
Darlington emitter-follower: R1 = 10 kΩ, R2 = 22 kΩ, RE = 22Ω, RL = 8Ω, VCC = 12V, βac =βDC =100.
The Common-collector Amplifier – contd.
2E2 DC
B CC2E1 2 DC
|| 20 12V = 8.0V30||R RV V
R R Rββ
⎛ ⎞ ⎛ ⎞⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎜ ⎟⎜ ⎟ ⎝ ⎠⎝ ⎠
= =+
E B BEE
E E
2 6.6V 300mA22V V VI R R
−= = = =Ω
'
E
25mV 25mV 83m300mAer I= = = Ω
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₪ Example 6-10 – contd. The load of the CE amplifier is Rin(tot) of the EF.
The voltage gain of
the common-emitter amplifier
The voltage gain of the Darlington EF
The overall voltage gain
The Common-collector Amplifier – contd.
1 2( ) ( )2 '
1 22
|| ||
|| || ( )10k || 22k ||100 (83m 5.87 ) 860
in tot in base
ac e e
R R R R
R R r Rβ
=
= += Ω Ω Ω + Ω = Ω
'860 1725
cve
RAr
= = =
'5.87 0.9983m 5.87
eve e
RAr R
= = =Ω ++
'(EF) (CE) (0.99)(172) 170v v vA A A= = =
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₪ The Sziklai Pair
The Common-collector Amplifier – contd.
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₪ Voltage Gain Notice that there is no phase inversion bet. output and input.
The Common-base Amplifier
' '( || ) ( || )out c c cv
e e ein E E
V I R RA V I r R r R= = ≅
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₪ Input Resistance The resistance, looking in at the emitter
₪ Output Resistance The resistance, looking in at the collector
₪ Current Gain
The Common-base Amplifier –contd.
''
( )( || ) ( || )e ein e E e Ein emitter e ein
I r RV VR r RI I I= = = =
'C C||coutR r R R= ≅
1out ci ein
I IA I I= = ≅
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₪ Multistage Voltage Gain
Multistage Amplifiers
'1 2 3v vnv v vA A A A A= L
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₪ Capacitively-coupled Multistage Amplifier
Multistage Amplifiers – contd.
51 3 6 ( 2)|| || || 1.63kc in baseR R R R R= = Ω
' 'E 1( 2)
E
25mV1.05mA, 23.8 , and 3.57ke eacin baseI r R rI β= = = Ω = = Ω
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₪ Capacitively-coupled Multistage Amplifier
The overall Voltage Gain
Multistage Amplifiers – contd.
11 ' 68.5c
ve
RAr
= =
72 '
4.7k 19723.8ve
RAr
Ω= = =Ω
'1 2 (68.5)(197) 13,495v v vA A A= = =
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₪ Direct-coupled Multistage Amplifier Advantages
No coupling capacitors
Can amplify low frequencies
Down to dc (0 Hz).
Disadvantage Affected by the changes due
to temperature.
Multistage Amplifiers – contd.
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₪ Explained the Amplifier Operation
₪ Explained the BJT AC Models
₪ Introduced the Common-emitter Amplifier
₪ Introduced the common-base amplifier
₪ Introduced the common-collector amplifier
₪ Discussed the operation of multi-stage amplifiers
Class Summary
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Discussion & Notes
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