Lect 4 BJT AC Analysis (Common Emitter Amplifier AC
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Transcript of Lect 4 BJT AC Analysis (Common Emitter Amplifier AC
LECTURER 4LECTURER 4LECTURER 4LECTURER 4
BJT AC ANALYSIS BJT AC ANALYSIS BJT AC ANALYSIS BJT AC ANALYSIS
Semester II 2010/11Semester II 2010/11Semester II 2010/11Semester II 2010/11
BJT AC ANALYSIS BJT AC ANALYSIS BJT AC ANALYSIS BJT AC ANALYSIS
(COMMON EMITTER AMPLIFIERS (COMMON EMITTER AMPLIFIERS (COMMON EMITTER AMPLIFIERS (COMMON EMITTER AMPLIFIERS AC LOADLINE)AC LOADLINE)AC LOADLINE)AC LOADLINE)
School of Microelectronic Engineering School of Microelectronic Engineering School of Microelectronic Engineering School of Microelectronic Engineering
((((SoMeSoMeSoMeSoMe) ) ) )
UniversitiUniversitiUniversitiUniversiti Malaysia PerlisMalaysia PerlisMalaysia PerlisMalaysia Perlis
AC LOAD LINE ANALYSIS
R1RC
VCC vO
RS
RC RL
NoteNoteNoteNote: The DC & AC load line analysis will be based on these circuits
RS
R1
R2 RE
RL
vs
vO
CC1
CC2 vs R1 || R2RE
RL
Common-emitter amplifier with emitter resistor
AC equivalent circuit
AC LOAD LINE ANALYSIS - DC Load Line
•KVL at C-E loop
ECCCCE
EECCCECC
RIRIV
RIRIVV
+
+++=
++=
1
1
β
β
β
DC Load Line
EC
ECCQCEQCC
ECCQCEQCC
RR
RRIVV
RRIVV
+=
+=−
++=
≅+
1- Slope
)(
)(
11 assume point, -QFor
β
β
AC LOAD LINE ANALYSIS - AC Load Line
AC Load Line
DC Load Line
Common-Emitter Amplifier with Emitter Bypass Capacitor
RS
R1RC
vO
VCC
Emitter bypass capacitor, CEmitter bypass capacitor, CEmitter bypass capacitor, CEmitter bypass capacitor, CEEEE
provides a provides a provides a provides a short circuitshort circuitshort circuitshort circuit to to to to ground for the ac signalsground for the ac signalsground for the ac signalsground for the ac signals
R2 RE
vs
CC
CE
Vo
Vs RC
RS
rπ roR1|| R2 gmVπSmallSmallSmallSmall----signal signal signal signal hybridhybridhybridhybrid----ππππequivalent circuitequivalent circuitequivalent circuitequivalent circuit
Note: Calculation examples in Neamen (Example 6.7)
Common-Emitter Amplifier with Emitter Bypass Capacitor
By include RE, it provide stability of Q-point.
If RE is too high +++> small-signal voltage gain will be reduced severely. (see Av equation)
Thus, RE is split to RE1 & RE2 and the second resistor is bypassedwith “emitter bypass capacitor”. CE provides a short circuit to ground for ac signal.
So, only RE1 is a part of ac equivalent circuit.
For dc stability: RE=RE1+RE2 For ac gain stability: RE=RE1 since CE will short RE2 to ground.
AC LOAD LINE ANALYSIS
NoteNoteNoteNote: The next DC & AC load line analysis will be
CommonCommonCommonCommon----emitteremitteremitteremitter amplifier with emitter bypass capacitoramplifier with emitter bypass capacitoramplifier with emitter bypass capacitoramplifier with emitter bypass capacitor
analysis will be based on this circuit
AC LOAD LINE ANALYSIS - DC Load Line
KVL on C-E loop
21
21
1 when ,)(
1
)(
CEEECCECC
EEECECC
IIVRRIVRI
VRRIVRIV
+=++
+++=
++++=
−
−+
β
β
β
β
21
21
21
1 Slope
)( So,
11
1, when point,-QFor
)(1
EEC
EECCQCEQ
EECCCCE
RRR
-
RRRIVVV
RRIRIVVV
++=
+++=−−+
≅
+>>
+
+++=−
−+
β
ββ
β
β
AC LOAD LINE ANALYSIS - AC Load Line
KVL on C-E loop
1
Assuming
0
ec
EeceCc
ii
RivRi
≅
=++
1
11
1- Slope
)(
EC
ECcEcCcce
RR
RRiRiRiv
+=
+−=+−=
AC equivalent circuit
NoteNoteNoteNote: The plot for DC & AC load line for this circuit is in Neamen (Figure 6.42)
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 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
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)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
Maximum Symmetrical Swing
Example:Determine the maximum symmetrical swing in the output voltage of the circuit given in Figure 6.43 (Neamen) (Note: RC = 5 kΩ, RL = 2 kΩ)
Solution: Solution:
Calculate the values or draw the dc load line. Calculate the values or draw the ac load line (resulting plot in Figure 6.44).
From the dc & ac load line, the maximum negative swing in the Ic is from 0.894 mA to zero (ICQ).
Maximum Symmetrical Swing
Example (cont)
So, the max possible peak-to-peak ac collector current:
mA 79.1)894.0(2
(min)),(2
==
−=∆ CCQc IIi
The max. symmetrical peak-to-peak output voltage:
Max instantaneous collector current:
V 56.2)2||5)(79.1()||(||
||||
==∆=
∆=∆
LCc
eqcce
RRi
Riv
mA 79.1894.0894.0||2
1=+=∆+= cCQC iIi