ANALOG ELECTRONIC CIRCUITS 1 EKT 204 Basic BJT Amplifiers (Part 2) 1.
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Transcript of ANALOG ELECTRONIC CIRCUITS 1 EKT 204 Basic BJT Amplifiers (Part 2) 1.
ANALOG ELECTRONIC CIRCUITS 1
EKT 204
Basic BJT Amplifiers (Part 2)
1
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
2
Common-Emitter Amplifier with Emitter Resistor
CE amplifier with emitter resistor Small-signal equivalent circuit (with current gain parameter, β)
inside transistor
3
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
4
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
15
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
6
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
7
Common Emitter Amplifier with emitter bypass capacitor
Common-emitter amplifier with emitter bypass capacitor
Example 1
8
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...
9
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...
10
DC & AC Load Lines
Full solution
11
AC LOAD LINE ANALYSISDetermine the dc and ac load line. VBE=0.7V, β=150, VA=∞
Example 2
12
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(
13
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
14
DC & AC Load lines
Full solution
15
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
16
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
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
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.
19
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
20