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Chapter 2 BJT Amplifiers

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Electronic Circuits
Chapter 2: BJT Amplifiers
1
Content
1. Device Structure and Physical Operation (Session 6.1)
2. Current–Voltage Characteristics (Session 6.2)
3. BJT Circuits at DC (Session 6.3)
4. Small-Signal Operation and Models
5. BJT Amplifier Configurations
2
1. Device Structure and Physical Operation
Review
3
2. Current–Voltage Characteristics
Circuit Symbols and Conventions
Circuit symbols for BJTs.
Voltage polarities and current flow in
transistors operating in the active mode.
4
2. Current–Voltage Characteristics
Circuit Symbols and Conventions
5
2. Current–Voltage Characteristics
The Common-Emitter Current Gain β
6
2. Current–Voltage Characteristics
Graphical Representation of Transistor Characteristics
The iC–vBE characteristic for an npn
transistor.
7
2. Current–Voltage Characteristics
8
2. Current–Voltage Characteristics
Large-signal, equivalent-circuit models of an npn BJT operating in the active mode in the
common-emitter configuration with the output resistance ro included.
9
3. BJT Circuits at DC
A Note on Units Except when otherwise specified, throughout this book we use a consistent set
of units, namely, volts (V), milliamps (mA), and kilohms (k ๏—)
3. BJT Circuits at DC
6Example
Active mode (npn BJT)
For modern npntransistors, ๐›ฝ is in the range 50 to 200, but it can be as high as
1000 for special devices.
Example 1:
The transistor in the following circuit having ๐›ฝ = 100
and exhibits a ๐‘ฃ๐ต๐ธ of 0.7๐‘‰ at ๐‘–๐ถ = 1 ๐‘š๐ด. Design the
circuit so that a current of 2๐‘š๐ด flows through the
collector and a voltage of +5 ๐‘‰ appears at the collector.
12
Active mode (npn BJT)
Example 2: In the circuit shown in figure a, the voltage at the emitter was measured
and found to be – 0.7 ๐‘‰. If ๐›ฝ = 50, find ๐ผ๐ธ , ๐ผ๐ต , ๐ผ๐ถ and ๐‘‰๐ถ .
Example 3: In the circuit shown
in figure b, measurement
indicates ๐‘‰๐ต to be +1.0๐‘‰ and ๐‘‰๐ธ
to be +1.7๐‘‰. What are ๐›ผ and ๐›ฝ
for this transistor? What voltage
๐‘‰๐ถ do we expect at the collector?
Figure a
Figure b
13
Transistor Characteristics
๐‘–๐ถ - ๐‘ฃ๐ต๐ธ characteristic for an npn transistor.
14
Transistor Characteristics – Early Effect
๐‘–๐ถ - ๐‘ฃ๐ถ๐ต characteristic for an npn transistor.
๐‘ฝ๐‘จ : Early Voltage.
๐‘ฝ๐‘จ ~ 10V – 100V.
15
Transistor Characteristics – Early Effect
In saturation region, it behaves as a closed switch with a small resistance ๐‘…๐ถ๐ธ๐‘ ๐‘Ž๐‘ก .
The saturation I-V curve can be approximated by a straight line intersecting the
๐‘ฃ๐ถ๐ธ axis at ๐‘‰๐ถ๐ธ๐‘œ๐‘“๐‘“ .
The
output
resistance
looking into the collector is
not infinite:
๐’“๐’ =
๐‘ฝ๐‘จ + ๐‘ฝ๐‘ช๐‘ฌ
๐‘ฐ๐‘ช
16
BJT Circuits at DC - npn
• Step 1: assume the operation mode.
• Step 2: use the conditions or model for circuit analysis.
• Step 3: verify the solution.
• Step 4: repeat the above steps with another assumption if necessary.
17
BJT Circuits at DC - npn
Example 4: Analyze the following circuit to
determine all node voltages and branch currents.
Assume that β is specified to be 100.
18
BJT Circuits at DC - npn
Example 5: Analyze the circuit in Example 1 to determine all node voltages and branch
currents. The voltage at the base is now +0V.
19
BJT Circuits at DC - npn
Example 6: Analyze the circuit in Example 1 to determine all node voltages and branch
currents. The voltage at the base is now +6V.
20
BJT Circuits at DC - pnp
21
BJT Circuits at DC
Example 7: Analyze the following circuit to
determine all node voltages and branch currents.
Assume that β is specified to be 100.
22
BJT Circuits at DC
Example 8: Analyze the following circuit to determine all node voltages and branch
currents. Assume that β is specified to be 100.
23
BJT Circuits at DC
Example 9: Analyze the following circuit to determine all node voltages and branch
currents.
24
BJT Circuits at DC
Example 10: Analyze the following circuit to determine all node voltages and branch
currents. Assume that β is specified to be 100.
25
DC Bias for BJT amplifier
โ– The amplifiers are operating at a proper dc bias point.
โ– The DC bias circuit is to ensure the BJT in active mode with a proper collector current IC.
Point Q is known as the bias point
or the dc operating point.
The signal to be amplified ๐‘ฃ๐‘๐‘’ ,a
function of time ๐‘ก.
๐‘‰๐ถ๐ธ = ๐‘‰๐ถ๐ถ − ๐‘…๐ถ ๐ผ๐‘†
๐‘‰๐ต๐ธ
เต—๐‘‰
๐‘‡
๐‘’
26
DC Bias for BJT amplifier
The signal to be amplified ๐‘ฃ๐‘๐‘’ , a function of time ๐‘ก:
๐’—๐‘ฉ๐‘ฌ ๐’• = ๐‘ฝ๐‘ฉ๐‘ฌ + ๐’—๐’ƒ๐’† (๐’•)
27
DC
Bias
for
BJT
amplifier
โ– The classical discrete-circuit bias arrangement:
โžข A single power supply and resistors are needed.
28
DC Bias for BJT amplifier
โ– The classical discrete-circuit bias arrangement:
โžข The two-power-supply version.
29
DC Bias for BJT amplifier
โ– Biasing using a constant-current source:
โžข RC is chosen to operate the BJT in active mode.
โžข The current source is typically implemented by a BJT current mirror.
โœ“ Both BJT transistors Q1 and Q2 are in active mode.
โœ“Assume current gain ๏ข is very high.
I REF
VCC + VEE − VBE
=
R
30
DC Bias for BJT amplifier
โ– Biasing using a collector-to-base feedback resistor:
โžข RB ensures the BJT in active (VCE > VBE = 0.7V)
31
Obtaining a Voltage Amplifier
The output voltage ๐‘ฃ๐ถ๐ธ is given by:
In active mode:
The result is:
๐’—๐‘ช๐‘ฌ = ๐‘ฝ๐‘ช๐‘ช − ๐’Š๐‘ช ๐‘น๐‘ช
๐’Š๐‘ช = ๐‘ฐ ๐‘บ
๐’—๐‘ฉ๐‘ฌ
เต—๐‘ฝ
๐‘ป
๐’†
๐’—๐‘ช๐‘ฌ = ๐‘ฝ๐‘ช๐‘ช −
(Neglect the Early effect)
๐’—๐‘ฉ๐‘ฌ
เต—๐‘ฝ
๐‘ป๐‘น
๐‘ฐ๐‘บ ๐’†
๐‘ช
This is obviously a nonlinear relationship.
32
Biasing the BJT
A dc voltage is selected to obtain operation at a point Q: ๐‘ฝ๐‘ช๐‘ฌ = ๐‘ฝ๐‘ช๐‘ช −
๐‘ฝ๐‘ฉ๐‘ฌ
เต—๐‘ฝ
๐‘ป๐‘น
๐‘ฐ๐‘บ ๐’†
๐‘ช
Point Q is known as the Bias point or the DC operating point.
Since at Q no signal component is present, it is also known as the Quiescent point.
33
Biasing the BJT
The signal ๐‘ฃ๐‘๐‘’ to be amplified a
function of time ๐‘ก is superimposed on
the bias voltage ๐‘‰๐ต๐ธ :
๐’—๐‘ฉ๐‘ฌ ๐’• = ๐‘ฝ๐‘ฉ๐‘ฌ + ๐’—๐’ƒ๐’† (๐’•)
The resulting ๐‘ฃ๐ถ๐ธ (๐‘ก) can be obtained
by substituting this expression for
๐’—๐‘ฉ๐‘ฌ ๐’• into:
๐’Š๐‘ช = ๐‘ฐ ๐‘บ
๐’—๐‘ฉ๐‘ฌ
เต—๐‘ฝ
๐‘ป
๐’†
34
Small-Signal Operation and Models
We consider the DC bias conditions by setting ๐’—๐’ƒ๐’† = ๐ŸŽ. Then:
๐‘ฐ ๐‘ช = ๐‘ฐ๐‘บ
๐‘ฐ๐‘ฌ =
๐‘ฝ๐‘ฉ๐‘ฌ
เต—๐‘ฝ
๐‘ป
๐’†
๐‘ฐ๐‘ฉ =
๐‘ฐ๐‘ชเต—
๐œถ
๐‘ฐ๐‘ช
เต—๐œท
๐‘ฝ๐‘ช๐‘ฌ = ๐‘ฝ๐‘ช๐‘ช − ๐‘ฐ๐‘ช ๐‘น๐‘ช
When ๐’—๐’ƒ๐’† ≠ ๐ŸŽ , the total instantaneous base-emitter voltage
๐’—๐‘ฉ๐‘ฌ becomes: ๐’—๐‘ฉ๐‘ฌ = ๐‘ฝ๐‘ฉ๐‘ฌ + ๐’—๐’ƒ๐’†
The collector current becomes:
๐’Š๐‘ช = ๐‘ฐ๐‘บ ๐’†๐’—๐‘ฉ๐‘ฌΤ๐‘ฝ๐‘ป = ๐‘ฐ๐‘บ ๐’†๐‘ฝ๐‘ฉ๐‘ฌΤ๐‘ฝ๐‘ป ๐’†๐’—๐’ƒ๐’† Τ๐‘ฝ๐‘ป = ๐‘ฐ๐‘ช ๐’†๐’—๐’ƒ๐’† Τ๐‘ฝ๐‘ป
Small signal operation: ๐’—๐’ƒ๐’† โ‰ช ๐‘ฝ๐‘ป
๐’Š๐‘ช = ๐‘ฐ ๐‘ช + ๐’Š๐’„ ≈ ๐‘ฐ ๐‘ช ๐Ÿ +
๐’—๐’ƒ๐’†
๐‘ฐ๐‘ช
= ๐‘ฐ๐‘ช +
๐’—
๐‘ฝ๐‘ป
๐‘ฝ๐‘ป ๐’ƒ๐’†
๐››๐’Š๐‘ช
๐‘ฐ๐‘ช
๐’ˆ๐’Ž =
|
=
๐››๐’—๐‘ฉ๐‘ฌ ๐’Š๐‘ช =๐‘ฐ๐‘ช ๐‘ฝ๐‘ป
35
Small-Signal Operation and Models
gm is called the trans-conductance:
๐››๐’Š๐‘ช
๐‘ฐ๐‘ช
๐’ˆ๐’Ž =
|
=
๐››๐’—๐‘ฉ๐‘ฌ ๐’Š๐‘ช =๐‘ฐ๐‘ช ๐‘ฝ๐‘ป
36
Small-Signal Operation and Models
โ– The base current and the input resistance at the base:
โžข Base current:
๐’Š๐‘ช ๐‘ฐ๐‘บ ๐’— Τ๐‘ฝ
๐’Š๐‘ฉ = = ๐’† ๐‘ฉ๐‘ฌ ๐‘ป = ๐‘ฐ๐‘ฉ ๐’†๐’—๐’ƒ๐’† Τ๐‘ฝ๐‘ป
๐œท
๐œท
โžข Small-signal approximation: ๐‘ฃ๐‘๐‘’ << ๐‘‰๐‘‡
๐’Š๐‘ฉ = ๐‘ฐ ๐‘ฉ + ๐’Š๐’ƒ ≈ ๐‘ฐ ๐‘ฉ ๐Ÿ +
๐’—๐’ƒ๐’†
๐œท
๐‘ฝ๐‘ป
๐’“๐… =
=
=
๐’Š๐’ƒ
๐’ˆ๐’Ž ๐‘ฐ ๐‘ฉ
๐’—๐’ƒ๐’†
๐‘ฐ๐‘ฉ
= ๐‘ฐ๐‘ฉ +
๐’—
๐‘ฝ๐‘ป
๐‘ฝ๐‘ป ๐’ƒ๐’†
The small-signal input
resistance between base and
emitter (looking into the base)
37
Small-Signal Operation and Models
โ– The emitter current and the input resistance at the emitter:
โžข Emitter current:
๐’Š๐‘ฌ = ๐‘ฐ ๐‘ฌ + ๐’Š๐’† =
๐’Š๐‘ช ๐‘ฐ ๐‘ช ๐’Š๐’„
= +
๐œถ
๐œถ ๐œถ
โžข Small-signal approximation: ๐‘ฃ๐‘๐‘’ << ๐‘‰๐‘‡
๐’Š๐’„ ๐’ˆ๐’Ž
๐‘ฐ๐‘ฌ
=
๐’—๐’ƒ๐’† =
๐’—
๐œถ
๐œถ
๐‘ฝ๐‘ป ๐’ƒ๐’†
๐’—๐’ƒ๐’† ๐‘ฝ๐‘ป
๐œถ
๐Ÿ
๐’“๐’† ≡
=
=
≈
๐’Š๐’†
๐‘ฐ ๐‘ฌ ๐’ˆ๐’Ž ๐’ˆ๐’Ž
๐’Š๐’† =
๐’“๐… = ๐Ÿ + ๐œท ๐’“๐’†
The relation between resistance
at base and resistance at emitter
38
Small-Signal Operation and Models
There are two type of equivalent circuit model of and BJT in small-signal operation:
โ–ช
The Hybrid-Pi model.
โ–ช
The T model.
Two models are exchangeable and does not affect the analysis result.
The hybrid-π model: typically used as the emitter is grounded.
39
Small-Signal Operation and Models
The T model: typically used as the emitter is not grounded.
40
Small-Signal Operation and Models
The analysis above indicates that every current and voltage in the amplifier circuit
is composed of two components: a dc component and a small-signal component.
• DC analysis:
• Remove all ac sources (short for voltage source and open for current source).
• All capacitors are considered open-circuit.
• DC analysis of BJT circuits for all nodal voltages and branch currents.
• Find the dc current ๐‘ฐ๐‘ช and make sure the BJT is in active mode.
• AC analysis:
• Remove all dc sources (short for voltage source and open for current source).
• All large capacitors are considered short-circuit.
• Replace the BJT with its small-signal model for ac analysis.
• The circuit parameters in the small-signal model are obtained based on the
value of ๐‘ฐ๐‘ช.
41
Small-Signal Operation and Models
Example 12:
a. Analyze the following transistor amplifier to determine its voltage gain ๐‘ฃ๐‘œΤ๐‘ฃ๐‘–.
Assume β = 100.
b. Assume that ๐‘ฃ๐‘– has a triangular waveform. Determine the maximum amplitude
that ๐‘ฃ๐‘– is allowed to have.
c. Set amplitude of ๐‘ฃ๐‘– to this value, give the waveforms of the total quantities
๐‘–๐ต(๐‘ก), ๐‘ฃ๐ต๐ธ (๐‘ก), ๐‘–๐ถ (๐‘ก), and ๐‘ฃ๐ถ (๐‘ก).
42
Small-Signal Operation and Models
Example 13: Analyze the following transistor amplifier to determine its voltage gain
๐‘ฃ๐‘œ
Τ๐‘ฃ๐‘–. Assume β = 100.
43
Small-Signal Operation and Models
Example 14: Calculate the overall voltage gain (๐‘ฃ๐‘œ/๐‘ฃ๐‘ ๐‘–๐‘”) of the following circuit. What is
the input resistance ๐‘…๐‘–๐‘›. Assume ๐›ฝ = 200.
44
Small-Signal Operation and Models
Example 15: Find the input resistance ๐‘…๐‘–๐‘ and ๐‘…๐‘–๐‘› and the overall voltage gain (๐‘ฃ๐‘œ/๐‘ฃ๐‘ ๐‘–๐‘”).
Assume ๐›ฝ = 200.
45
Small-Signal Analysis – Early Effect
Early effect: The collector current depends not only on ๐’—๐‘ฉ๐‘ฌ but also on ๐’—๐‘ช๐‘ฌ.
The dependence on ๐‘ฃ๐ถ๐ธ can be modeled by assigning a finite output resistance:
๐‘Ÿ๐‘œ = (๐‘‰๐ด + ๐‘‰๐ถ๐ธ )/๐ผ๐ถ ≈ ๐‘‰๐ด /๐ผ๐ถ (๐‘‰๐ด : the Early voltage).
46
Small-Signal Analysis – Early Effect
Early effect: The collector current depends not only on ๐’—๐‘ฉ๐‘ฌ but also on ๐’—๐‘ช๐‘ฌ.
The dependence on ๐‘ฃ๐ถ๐ธ can be modeled by assigning a finite output resistance:
๐‘Ÿ๐‘œ = (๐‘‰๐ด + ๐‘‰๐ถ๐ธ )/๐ผ๐ถ ≈ ๐‘‰๐ด /๐ผ๐ถ (๐‘‰๐ด : the Early voltage).
47
Small-Signal Analysis – Summary
48
โ–ช
Basic BJT Amplifier Configurations
Three basic configurations
49
Basic BJT Amplifier Configurations
Characterizing amplifiers:
•
๐’—
๐’Š๐’Š
Input resistance: ๐‘น๐’Š๐’ = ๐’Š. Together
with the resistance ๐‘น๐’”๐’Š๐’ˆ forms a
voltage divider that reduces ๐’—๐’”๐’Š๐’ˆ .
๐‘ฃ๐‘– = ๐‘ฃ๐‘ ๐‘–๐‘”
•
๐‘…๐‘–๐‘›
๐‘…๐‘–๐‘› + ๐‘…๐‘ ๐‘–๐‘”
Open circuit voltage gain:
๐‘จ๐’—๐ŸŽ =
๐’—๐’
แ‰ค
๐’—๐’Š ๐‘น
๐‘ณ =∞
50
Basic BJT Amplifier Configurations
•
Output resistance: ๐‘น๐ŸŽ =
๐’—๐’™
๐’Š๐’™
The output voltage can be found from:
The overall voltage gain ๐‘ฎ๐’— :
๐‘น๐‘ณ
๐’—๐ŸŽ =
๐‘จ ๐’—
๐‘น๐‘ณ + ๐‘น๐’ ๐’—๐’ ๐’Š
๐’—๐’
๐‘น๐’Š๐’
๐‘น๐‘ณ
๐‘ฎ๐’— ≡
=
๐‘จ
๐’—๐’”๐’Š๐’ˆ ๐‘น๐’Š๐’ + ๐‘น๐’”๐’Š๐’ˆ ๐’—๐’ ๐‘น๐‘ณ + ๐‘น๐’
51
Basic BJT Amplifiers - CE Amplifier
•
Input resistance: ๐‘น๐’Š๐’ = ๐’“๐…
•
OC voltage gain: ๐‘จ๐’—๐’ = −๐’ˆ๐’Ž ๐‘น๐‘ช โˆฅ ๐’“๐’
•
Output resistance: ๐‘น๐’ = ๐‘น๐‘ช โˆฅ ๐’“๐’
•
Overall voltage gain: ๐‘ฎ๐’— =
๐’—๐’
๐’—๐’”๐’Š๐’ˆ
=−
๐’“๐…
๐’ˆ
๐’“๐… +๐‘น๐’”๐’Š๐’ˆ ๐’Ž
๐‘น๐‘ช โˆฅ ๐‘น๐‘ณ โˆฅ ๐’“ ๐’
52
Basic BJT Amplifiers - CE Amplifier
Alternative Gain expression:
•
Voltage gain:
๐ด๐‘ฃ = −๐‘”๐‘š ๐‘…๐ฟ โˆฅ ๐‘…๐ถ โˆฅ ๐‘Ÿ๐‘œ = −๐›ผ
•
๐‘…๐ฟ โˆฅ ๐‘…๐ถ โˆฅ ๐‘Ÿ๐‘œ
๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ ๐‘Ÿ๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘Ž๐‘›๐‘๐‘’ ๐‘–๐‘› ๐‘๐‘œ๐‘™๐‘™๐‘’๐‘๐‘ก๐‘œ๐‘Ÿ
= −๐›ผ
๐‘Ÿ๐‘’
๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ ๐‘Ÿ๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘Ž๐‘›๐‘๐‘’ ๐‘–๐‘› ๐‘’๐‘š๐‘–๐‘ก๐‘ก๐‘’๐‘Ÿ
Overall voltage gain:
๐บ๐‘ฃ = −
๐‘Ÿ๐œ‹
๐‘…๐ฟ โˆฅ ๐‘…๐ถ โˆฅ ๐‘Ÿ๐‘œ
๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ ๐‘Ÿ๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘Ž๐‘›๐‘๐‘’ ๐‘–๐‘› ๐‘๐‘œ๐‘™๐‘™๐‘’๐‘๐‘ก๐‘œ๐‘Ÿ
๐‘”๐‘š ๐‘…๐ฟ โˆฅ ๐‘…๐ถ โˆฅ ๐‘Ÿ๐‘œ = −๐›ฝ
= −๐›ฝ
๐‘Ÿ๐œ‹ + ๐‘…๐‘ ๐‘–๐‘”
๐‘…๐‘ ๐‘–๐‘” + ๐‘Ÿ๐œ‹
๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ ๐‘Ÿ๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘Ž๐‘›๐‘๐‘’ ๐‘–๐‘› ๐‘๐‘Ž๐‘ ๐‘’
Example 16: A CE amplifier utilizes a BJT with ๐›ฝ = 100 and ๐‘‰๐ด = 100๐‘‰, is biased at
๐ผ๐ถ = 1mA and has a collector resistance ๐‘…๐ถ = 5๐‘˜Ω. Find ๐‘…๐‘–๐‘› , ๐‘…๐‘œ and ๐ด๐‘ฃ๐‘œ . If the
amplifier is fed with a signal source having a resistance of 5๐‘˜Ω and a load resistance
๐‘…๐ฟ = 5๐‘˜Ω is connected to the output terminal, find the resulting ๐ด๐‘ฃ and ๐บ๐‘ฃ If ๐‘ฃเทœ๐œ‹ is to
be limited to 5 mV, what are the corresponding ๐‘ฃเทœ๐‘ ๐‘–๐‘” and ๐‘ฃเทœ๐‘œ with the load connected?
53
Basic BJT Amplifiers - CE Amplifier
CE Amplifier with Emitter Resistance:
•
Input resistance:
๐‘น๐’Š๐’ = ๐œท + ๐Ÿ ๐’“๐’† + ๐‘น๐’†
•
OC voltage gain:
๐‘จ๐’—๐’
•
๐‘น๐‘ช
= −๐œถ
๐’“๐’† + ๐‘น๐’†
Overall voltage gain:
๐‘ฎ๐’— = −
๐‘น๐’Š๐’
๐‘น๐‘ช โˆฅ ๐‘น๐‘ณ
๐œถ
๐‘น๐’Š๐’ + ๐‘น๐’”๐’Š๐’ˆ ๐’“๐’† + ๐‘น๐’†
1.
๐‘น๐’Š๐’ is increased by ๐Ÿ + ๐’ˆ๐’Ž ๐‘น๐’†
2.
๐‘จ๐’— is decreased by ๐Ÿ + ๐’ˆ๐’Ž ๐‘น๐’†
54
Basic BJT Amplifiers - CE Amplifier
Example 17: For the CE amplifier specified in Example 16, what value of ๐‘…๐‘’ is needed to
raise ๐‘…๐‘–๐‘› to a value four times that of ๐‘…๐‘ ๐‘–๐‘” ? With included ๐‘…๐‘’ , find ๐ด๐‘ฃ๐‘œ , ๐‘…๐‘œ and ๐ด๐‘ฃ and
๐บ๐‘ฃ . Also, if ๐‘ฃเทœ๐œ‹ is limited to 5 mV, what are the corresponding values of ๐‘ฃเทœ๐‘ ๐‘–๐‘” and ๐‘ฃเทœ๐‘œ ?
55
Basic BJT Amplifiers - CB Amplifier
•
Input resistance: ๐‘…๐‘–๐‘› = ๐‘Ÿ๐‘’
•
OC voltage gain: ๐ด๐‘ฃ๐‘œ = ๐‘”๐‘š ๐‘…๐ถ
•
Output resistance: ๐‘…๐‘œ = ๐‘…๐ถ
•
Overall voltage gain: ๐บ๐‘ฃ =
๐‘ฃ๐‘œ
๐‘ฃ๐‘ ๐‘–๐‘”
=
๐‘Ÿ๐‘’
๐‘”
๐‘Ÿ๐‘’ +๐‘…๐‘ ๐‘–๐‘” ๐‘š
๐‘…๐ถ โˆฅ ๐‘…๐ฟ
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Basic BJT Amplifiers - CC Amplifier
The need for voltage buffers: the amplifier has
•
High input resistance.
•
Low output resistance.
57
Basic BJT Amplifiers - CC Amplifier
•
Input resistance: ๐‘…๐‘–๐‘› = ๐›ฝ + 1 ๐‘Ÿ๐‘’ + ๐‘…๐ฟ
•
Voltage gain:
•
Output resistance: ๐‘…๐‘œ = ๐‘Ÿ๐‘’
•
Overall voltage gain: ๐บ๐‘ฃ =
๐ด๐‘ฃ =
๐‘…๐ฟ
๐‘…๐ฟ +๐‘Ÿ๐‘’
๐‘ฃ๐‘œ
๐‘ฃ๐‘ ๐‘–๐‘”
≈1
=
๐›ฝ+1 ๐‘…๐ฟ
๐›ฝ+1 ๐‘…๐ฟ + ๐›ฝ+1 ๐‘Ÿ๐‘’ +๐‘…๐‘ ๐‘–๐‘”
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Basic BJT Amplifiers - CC Amplifier
Example 18: It is required to design an emitter follower to implement the buffer
amplifier of following figure. Specify the required bias current ๐ผ๐ธ and the minimum
value ๐›ฝ the transistor must have. Determine the maximum allowed value of ๐‘ฃ๐‘ ๐‘–๐‘” if ๐‘ฃ๐œ‹ is
to be limited to 5๐‘š๐‘‰ in order to obtain reasonably linear operation. With ๐‘ฃ๐‘ ๐‘–๐‘” =
200๐‘š๐‘‰, determine the signal voltage at the output if ๐‘…๐ฟ is changed to 2๐‘˜Ω and to
0.5๐‘˜Ω.
59
Basic BJT Amplifiers - Summary
60
Basic BJT Amplifiers
Example 19: For the following
circuit, let ๐‘‰๐ถ๐ถ = 9V, ๐‘…1 =
27๐‘˜Ω , ๐‘…2 = 15๐‘˜Ω , ๐‘…๐ธ =
1.2๐‘˜Ω, and ๐‘…๐ถ = 2.2๐‘˜Ω. The
transistor has ๐›ฝ = 100 .
Calculate the DC bias current
๐ผ๐ธ . If the amplifier operates
between a source for which
๐‘…๐‘ ๐‘–๐‘” = 10๐‘˜Ω and a load
of 2๐‘˜Ω. Find the value of ๐‘…๐‘–๐‘›,
the voltage gain ๐‘ฃ๐‘œ/๐‘ฃ๐‘ ๐‘–๐‘”.
61
Graphical analysis
62
DC Load Line
63
DC Load Line
64
AC Load Line
65
AC Load Line
•
Max swing condition:
๐‘ฐ๐‘ช๐‘ธ
๐‘ฝ๐‘ช๐‘ช
=
๐‘น๐‘ซ๐‘ช + ๐‘น๐’‚๐’„
66
Exercises
Exercise 1: In the following circuit, ๐‘ฃ๐‘ ๐‘–๐‘” is a small sine wave signal with zero average.
The transistor β is 100.
a. Find the value of ๐‘…๐ธ to establish a dc emitter current of about 0.5 mA.
b. Find ๐‘…๐ถ to establish a dc collector voltage of about +5 V.
c. For๐‘…๐ฟ = 10 ๐‘˜Ω and ๐‘Ÿ๐‘œ = 200๐‘˜Ω, draw the
small-signal equivalent circuit of the amplifier
and determine its overall voltage gain.
67
Exercises
Exercise 2: Using the topology of following circuit, design an amplifier to operate
between a 10๐‘˜Ω source and a 2๐‘˜Ω load with a gain of −8๐‘‰/๐‘‰. The power supply
available is 9๐‘‰. Use an emitter current of approximately 2๐‘š๐ด and a current of about
one-tenth of that in the voltage divider that feeds the base, with the dc voltage at the
base about one-third of the supply. The transistor available has ๐›ฝ = 100 and ๐‘‰๐ด =
100๐‘‰. Use standard 5% resistor.
68
Exercises
Exercise 3: The following amplifier consists of two identical common-emitter
amplifiers connected in cascade. Observe that the input resistance of the second
stage, ๐‘…๐‘–๐‘›2, constitutes the load resistance of the first stage.
a. For ๐‘‰๐ถ๐ถ = 15๐‘‰, ๐‘…1 = 100๐‘˜Ω, ๐‘…2 = 47๐‘˜Ω, ๐‘…๐ธ = 3.9๐‘˜Ω, ๐‘…๐ถ = 6.8๐‘˜Ω, and ๐›ฝ =
100, determine the DC collector current and voltage of each transistor.
b. Draw the small-signal equivalent circuit of the entire amplifier and give the values
of all its components.
c. Find ๐‘…๐‘–๐‘›1 and
๐‘ฃ๐‘1
เต—๐‘ฃ๐‘ ๐‘–๐‘” for ๐‘…๐‘ ๐‘–๐‘” =
5๐‘˜Ω.
d. Find ๐‘…๐‘–๐‘›2 and
๐‘ฃ๐‘2
Τ๐‘ฃ๐‘1
e. For ๐‘…๐ฟ = 2 ๐‘˜Ω,
find ๐‘ฃ๐‘œΤ๐‘ฃ๐‘2
f. Find the overall
voltage gain ๐‘ฃ๐‘œเต—๐‘ฃ๐‘ ๐‘–๐‘”
69
Exercises
Exercise 4: For the following emitter-follower circuit, the BJT used is specified to have
β values in the range of 40 to 200 (a distressing situation for the circuit designer). For
the two extreme values of β (β = 40 and β = 200), find:
a. ๐ผ๐ธ , ๐‘‰๐ธ , and ๐‘‰๐ต .
b. The input resistance ๐‘…๐‘–๐‘› .
c. The voltage gain ๐‘ฃ๐‘œเต—๐‘ฃ๐‘ ๐‘–๐‘” .
70
Q&A
71
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