BJT Biasing Circuits LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
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Base Bias •
VCC
RC
In a simple biasing circuit, VBB is eliminated by connecting the resistor RB to the supply VCC. VCC
RB VBB
RB
•
RC
As shown in the above circuit, two dc voltage supplies are needed to bias a BJT which is not practical. •
This biasing circuit is called base bias, or fixed bias.
LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
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VCC
RB
C B VBE
•
•
Since IC = βDCIB ,
IC =
IC
RC
IB
•
β DC (VCC -VBE ) RB
•
Applying KVL, VCC = ICRC + VCE
•
Therefore, VCE = VCC – ICRC
•
βDC varies from device to device resulting in the variation of IC. A good biasing circuit is to maintain a constant IC while βDC varies.
VCE E
Applying KVL, VCC = IBRB + VBE Therefore,
VCC -VBE IB = RB
•
LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
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DC Load Line •
IC
The dc load line is a graph that represents all the possible combinations of IC and VCE for a given BJT circuit.
IC(sat)
VCC
RB
IB
VCE(off)
IC
RC
A generic dc load line
C B VBE
VCE E
VCE
•
Ideally, Saturation: VCE = 0 VCC = IC R C IC(sat) =
LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
Cut-off: IC = 0 VCE(off) = VCC
VCC RC 4
Example 1: Plot the dc load line for the circuit shown below. +12 V
IC 2 kΩ
6 mA
RB
IC(sat) =
VCC 12 = = 6 mA R C 2k
12 V
VCE
The dc load line
VCE(off) = VCC = 12 V LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
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Q-Point +8 V
•
IC and VCE at Q-point are called ICQ and VCEQ respectively.
•
Determine IC and VCE if VBE is assumed to be 0.7 volt.
2 kΩ 360 kΩ
βDC = 100
•
• •
When a BJT does not have an ac input, it will have specific dc values of IC and VCE. These values will correspond to a specific point on the dc load line. This point is called the Q-point. The letter Q comes from the word quiescent, meaning at rest.
IC = =
β DC (VCC -VBE ) RB (100)(8-0.7) =2.028 mA 360k
VCE = VCC - IC R C = 8 - (2.028mA)(2k) = 3.94 V
LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
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•
Determine IC(sat) and VCE(off).
•
Construct the dc load line and plot the Q-point. IC
+8 V
2 kΩ
4 mA
360 kΩ
βDC = 100
2.028 mA
IC(sat)
3.94 V
V 8 = CC = = 4 mA R C 2k
VCE(off) = VCC = 8 V
Q
8V
VCE
The dc load line
•
The circuit is said to be midpoint biased since the values of IC and VCE at Q-point are one-half of their maximum values.
LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
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Feedback Bias: Collector-Feedback Bias VCC
•
Applying KVL,
VCC = VRC +VRB +VBE RC
= (IC +I B )R C +I B R B +VBE = β DC I B R C +I B R C +I B R B +VBE
RB
= (β DC +1)I B R C +I B R B +VBE
IC
IB
C B
VBE
VCE E
IB =
VCC -VBE R B +(β DC +1)R C
ICQ =
β DC (VCC -VBE ) R B +(β DC +1)R C
VCEQ = VCC - (ICQ +I B )R C ≈ VCC -ICQ R C ; β DC >> 1 LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
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Feedback Bias: Emitter-Feedback Bias VCC
•
Applying KVL,
RB
VCC = VRB +VBE + VRE IB
= I B R B +VBE + ( β DC + 1) I B RE
IC
RC
C B
VCE
IB =
VCC -VBE R B +(β DC +1)RE
ICQ =
β DC (VCC -VBE ) R B +(β DC +1)RE
E
VBE
VCEQ = VCC - ICQ R C + I E R E RE
IE
≈ VCC -ICQ (R C +R E ) ; β DC >> 1
LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
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Voltage-Divider Bias VCC
VCC RC
R1
IC
RC
I1
IB RBB
C IB
R2
I2
IC
VBB
B
VCE
VBE
RE
IE
E
RE
IE
• •
Replace circuit A with the thevenin equivalent circuit. Find VBB and RBB.
Circuit A LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
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VCC
VCC RC
IC
I1
R1
VBB = + I2
R2
IB
R1 VCC R1 +R 2
RBB VBB RE
IE
VBB=VOC -
•
Applying KVL, VBB = I B R BB + VBE + I E R E
R1
R BB = R1 // R 2 R2
= I B R BB + VBE + (β DC + 1)I B R E IB =
VBB - VBE R BB +(β DC + 1)R E
ICQ =
β DC (VBB - VBE ) R BB +(β DC +1)R E
RBB
VCEQ = VCC - (R C + R E )ICQ ; β DC >> 1 LE210 Lecture Notes 2002 Edition: BJT Biasing Circuits
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