Esercitazione amp-BJT.pps
-
Upload
luckyluke981 -
Category
Documents
-
view
216 -
download
0
Transcript of Esercitazione amp-BJT.pps
-
8/14/2019 Esercitazione amp-BJT.pps
1/22
1
Coupling and Bypass
Capacitors
AC coupling through capacitors isused to inject ac input signal andextract output signal without
disturbing Q-point
Capacitors provide negligibleimpedance at frequencies of interestand provide open circuits at dc.
C1and C3are large coupling capacitors
or dc blocking capacitors, their
reactance at signal frequency is
negligible.
C2is bypass capacitor, provides lowimpedance path for ac current from
emitter to ground, removingRE
(required for good Q-point stability)
from circuit when ac signals are
considered.
-
8/14/2019 Esercitazione amp-BJT.pps
2/22
2
DC and AC Analysis DC analysis:
Find dc equivalent circuit by replacing all capacitors by opencircuits and inductors by short circuits.
Find Q-point from dc equivalent circuit by using appropriate large-signal transistor model.
AC analysis:
Find ac equivalent circuit by replacing all capacitors by shortcircuits, inductors by open circuits, dc voltage sources by groundconnections and dc current sources by open circuits.
Replace transistor by small-signal model
Use small-signal ac equivalent to analyze ac characteristics ofamplifier.
Combine end results of dc and ac analysis to yield total voltagesand currents in the network.
-
8/14/2019 Esercitazione amp-BJT.pps
3/22
3
DC Equivalent for BJT Amplifier
All capacitors in original amplifier circuits are
replaced by open circuits, disconnecting vI,
RI, and R3from circuit.
-
8/14/2019 Esercitazione amp-BJT.pps
4/22
4
AC Equivalent for BJT Amplifier
k100k3.43
k30k1021
RC
RR
RRB
R
-
8/14/2019 Esercitazione amp-BJT.pps
5/22
5
Hybrid-Pi Model of BJT
The hybrid-pi small-signalmodel is the intrinsic low-frequency representation
of the BJT. Small-signal parameters
are controlled by the Q-point and are independentof geometry of BJT
Transconductance:
CI
TV
CI
mg 40
Input resistance:
mg
o
CI
TVo
r
Output resistance:
max)(guadagnoormgf
CIA
V
CI
CEV
AV
or
-
8/14/2019 Esercitazione amp-BJT.pps
6/22
6
Equivalent Forms of Small-
Signal Model for BJT
Voltage -controlled current source gmvbecan betransformed into current-controlled currentsource,
Basic relationship ic=ibis useful in both dc and
ac analysis when
BJT is in forward-active region.
bice
v
bici
bi
bi
bevbi
bev
oor
o
or
mg
mg
r
-
8/14/2019 Esercitazione amp-BJT.pps
7/22
7
Small-Signal Analysis of
Complete C-E Amplifier: AC
Equivalent Ac equivalent circuit
is constructed by
assuming that allcapacitances havezero impedance atsignal frequency and
dc voltage source isac ground.
Assume that Q-point
is already known.
21RR
BR
-
8/14/2019 Esercitazione amp-BJT.pps
8/22
8
Small-Signal Analysis of
Complete C-E Amplifier: Small-
Signal Equivalent
3R
CRorL
R
LRmg
bevov
bvcv
vtA
Terminal voltage gainbetween
base and collector is:
Overall voltage gain from source vi
to output voltage acrossR3is:
r
B
R
I
R
rB
R
LRmgvA
ivbev
vtA
ivbev
bevov
ivov
vA
-
8/14/2019 Esercitazione amp-BJT.pps
9/22
9
C-E Amplifier Voltage Gain:
Example Problem:Calculate voltage gain
Given data:F=100, VA=75 V, Q-point is (1.45 mA,
3.41 V), R1= 10 kW, R2= 30 kW,R3= 100 kW, RC=
4.3 kW, RI
= 1kW.
Assumptions:Transistor is in active region, O=
F. Signals are low enough to be considered small
signals.
C
be
Iic
mVv
%20
5
-
8/14/2019 Esercitazione amp-BJT.pps
10/22
10
Analysis
dB3.42130
rB
RI
R
rB
R
LRmgvA
mS0.58)mA45.1(4040 C
Img
k72.1mA45.1
)V025.0(100
CI
TVor
k1.54mA45.1
V14.3V75
C
ICE
VAV
or
k83.33 R
CRorL
Rk5.721 RR
BR
mV57.8
)(V)005.0(
rB
R
rB
RI
R
iv
i
BB
B
be
be
vrRR
rRv
mVv
)||(
||
5
-
8/14/2019 Esercitazione amp-BJT.pps
11/22
11
Small-Signal Model
Simplification If we assume
rBR
IR
3R
CRormgL
RmgvtAvA
This implies that total signal voltage at input
appears across r.
-
8/14/2019 Esercitazione amp-BJT.pps
12/22
12
Progetto amplificatore piccoli
segnali (carico resistivo)
Generally R3>> RCand R3
-
8/14/2019 Esercitazione amp-BJT.pps
13/22
13
C-E Amplifier Input Resistance
Input resistance, the totalresistance looking into the
amplifier at coupling
capacitor C1represents total
resistance presented tosource.
rRRrB
RR
rB
R
21
xixv
in
)(xixv
-
8/14/2019 Esercitazione amp-BJT.pps
14/22
14
C-E Amplifier Output Resistance
Output resistance is the total
equivalent resistance looking
into the output of the amplifier
at coupling capacitor C3. Input
source is set to 0 and test
source is applied at output.
CRorC
RR
mg
orCR
x
ixv
out
bevx
vxvxi but vbe=0
As ro>> R
C.
-
8/14/2019 Esercitazione amp-BJT.pps
15/22
15
Sample Analysis of C-E
Amplifier Problem:Find voltage gain, input
and output resistances.
Given data:F= 65, VA=50 V
Assumptions:Active-regionoperation, VBE=0.7 V, small signal
operatingconditions.
Analysis: To find the Q-point,dc equivalent circuit is
constructed.
A24566
A24165
A71.3
BI
EI
BI
CI
BI
5)4106.1()1(510 BI
FBEV
BI
V67.3
)4106.1(41055
CEV
EI
CEV
CI
jj
ji i IRV
KVL
S l A l i f C E
-
8/14/2019 Esercitazione amp-BJT.pps
16/22
16
Sample Analysis of C-E
Amplifier (contd.)
0.84
in
in)3out
(
RI
R
RRRmg
ivov
vA
S31064.940 C
Img
k64.6
C
IT
Vor
k223
CI
CEVAVor
k23.6
in
r
B
RR
k57.9out
orCRR
-
8/14/2019 Esercitazione amp-BJT.pps
17/22
17
CE senza Capacit di bypass
-
8/14/2019 Esercitazione amp-BJT.pps
18/22
18
Inverting Amplifiers: Terminal
Voltage Gain
Using test source vbto drive the base
terminal of the transistor, neglecting
ro,
ERL
R
ER
mg
LR
mg
ACEvt
ER
omg
o
L
R
o
ER
or
L
R
o
bvov
vtA
1
)1(/)1(
1oAssuming
Lamplificazione
dipende solo dai
resistori esterni!
LRmg
bevov
bvcv
vtA
Eob Rirv
KVL
)1(
-
8/14/2019 Esercitazione amp-BJT.pps
19/22
19
nver ng mp ers: npuResistance and Overall Voltage
Gain
mgro
o
1
Input resistance looking into the base
terminal is given by
)1(
)1(
ERmgrR
CEin
ERor
ibv
RCEin
RCEinBR
IR
RCEinBR
CEin
R
LRo
RCEinBR
IR
RCEinBR
ACEvt
ivbv
ACEvt
ivbv
bvov
ivov
ACEv
Overall voltage gain is
Assuming
Generatore reale! Av
rB
RI
R
rB
R
LRmgvA
iv
bev
vt
A
iv
bev
bev
ov
iv
ov
v
A
-
8/14/2019 Esercitazione amp-BJT.pps
20/22
20
Inverting Amplifiers: Output
Resistance
0ixi0i
0ev0)1(
1ev
i)1(ev
o
rth
RE
Ro
ERo
rthR
ev-
i
ButRout= rowhenRE= 0, not infinite.
Now, we also include roin our analysis.
xix
v
outR
rth
RE
RE
RoorR
rthRER
ER
ERr
thR
oro
1out
xii
xiev
ev)ixi(evrvxv
IBTH RRR //
CORTOCIRCUITANDO
IL GENERATORE DI
INGRESSO
neglect ing ro
-
8/14/2019 Esercitazione amp-BJT.pps
21/22
21
Inverting Amplifiers: Output
Resistance (contd.) rmgo Assuming and , with
.for
Finite current gain of BJT places an upper limit on size of output
resistance. rappears in parallel withREifRthis neglected. If we letREbe
infinite, maximum value of output resistance is
thR
ERr )( E
Ror
)()(out
)()(1out
ERr
fERrmgorR
ERr
for
ERrmgorR
1)(
E
Rrmg
oroR )1(out
CRorC
RR
xixv
out
Rout modifica Avperch RLdiventa il
parallelo tra il carico
e Rout
-
8/14/2019 Esercitazione amp-BJT.pps
22/22
22
Inverting Amplifiers: Current
Gain
oACE
it
ACEit rRR
R
i
rRRRi
i
i
i
iA
rRR
Rii
ii
EoB
B
i
EoB
BiO
i
O
i
Li
EoB
Bi
OL
)1(
)1(
)1(