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Chapter 3:
Bipolar Junction Transistors
Islamic University of Gaza
Dr. Talal Skaik
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Transistor Construction
2
Dr. Talal Skaik 2014
•The npn BJT consists of three semiconductor regions: the
emitter region (n type), the base region (p type), and the collector
region (n type).
•The pnp BJT consists of three semiconductor regions: the
emitter region (p type), the base region (n type), and the collector
region (p type).
There are two types of transistors:
• pnp
• npn
The terminals are labeled:
• E - Emitter
• B - Base
• C - Collector
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Transistor Construction
3
Dr. Talal Skaik 2014
The transistor consists of two pn junctions, the emitter–base
junction (EBJ) and the collector–base junction (CBJ).
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Transistor Construction
4
Dr. Talal Skaik 2014
Emitter: The portion on one side of transistor that supplies charge
carriers (i.e. electrons or holes) to the other two portions.
The emitter is a heavily doped region.
Emitter of PNP transistor supplies hole charges to its junction with
the base. Similarly, the emitter of NPN transistor supplies free
electrons to its junction with the base.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Transistor Construction
5
Dr. Talal Skaik 2014
Collector is the portion on the other side of the transistor (i.e. the
side opposite to the emitter) that collects the charge carriers (i.e.
electrons or holes).
The doping level of the collector is in between the heavily doping
of emitter and the light doping of the base.
Base: The middle portion which forms two PN junctions between
the emitter and the collector is called the base.
The base of transistor is thin, as compared to the emitter and is a
lightly doped portion.
The function of base is to control the flow of charge carrier.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
BJT Modes Of Operation
6
Dr. Talal Skaik 2014
There are two junctions in bipolar junction transistor.
Each junction can be forward or reverse biased independently.
Thus there are different modes of operations:
Forward Active.
Cut off.
Saturation.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
BJT Modes Of Operation
7
Dr. Talal Skaik 2014
FORWARD ACTIVE
Emitter-base junction is forward biased and collector-base
junction is reverse biased.
The BJT can be used as an amplifier and in analog circuits.
CUTT OFF
When both junctions are reverse biased it is called cut off mode.
In this situation there is nearly zero current and transistor behaves
as an open switch.
SATURATION
In saturation mode both junctions are forward biased.
Large collector current flows with a small voltage across collector
base junction.
Transistor behaves as an closed switch.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Operation of pnp transistor in active mode
8
Dr. Talal Skaik 2014
Reverse-biased junction of
a pnp transistor
Forward-biased junction of
a pnp transistor.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Operation of pnp transistor in active mode
9
Dr. Talal Skaik 2014
With the external sources, VEE and VCC, connected as shown:
• The emitter-base junction is forward biased
• The base-collector junction is reverse biased
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Currents in a Transistor
The collector current is comprised of two currents:
B
I
C
I
E
I 

minority
CO
I
majority
C
I
C
I 

Emitter current is the sum of the
collector and base currents:
10
Dr. Talal Skaik 2014
The minority current is called the leakage current and is given by
the symbol ICO (IC current with emitter terminal Open).
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Common Base Configuration
11
Dr. Talal Skaik 2014
The base is common to both
input (emitter–base) and
output (collector–base) of
the transistor.
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Common-Base Configuration
Input Characteristics
This curve shows the relationship
between of input current (IE) to
input voltage (VBE) for three output
voltage (VCB) levels.
12
Dr. Talal Skaik 2014
VBE=0.7 V
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
This graph demonstrates the output current (IC) to an output voltage
(VCB) for various levels of input current (IE).
Common-Base Configuration
Output Characteristics
13
Dr. Talal Skaik 2014
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Operating Regions
• Active – Operating range of the amplifier. It is noticed that IE
is approximately equal to IC (IC≈ IE ).
• Cutoff – the region where the collector current is
approximately 0A (IC=ICBO). The amplifier is basically off.
There is voltage, but little current.
• Saturation – Region to the left of VCB=0. Note the
exponential increase in collector current as the voltage VCB
increases toward 0 V. There is current but little voltage.
14
Dr. Talal Skaik 2014
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
E
I
C
I 
Silicon)
(for
V
0.7
BE
V 
Approximations
Emitter and collector currents:
Base-emitter voltage:
15
Dr. Talal Skaik 2014
Copyright ©2009 by Pearson Education, Inc.
Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/e
Robert L. Boylestad and Louis Nashelsky
Ideally: a = 1
In reality: a is between 0.9 and 0.998
Alpha (a)
Alpha (a) is the ratio of IC to IE :
E
I
C
I
α 
dc
Alpha (a) in the AC mode:
Δ
Δ constant
ac
IC
IE VCB
α


16
Dr. Talal Skaik 2014
E I
CBO
I αI
C  

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Chapter3 p1

  • 1. Chapter 3: Bipolar Junction Transistors Islamic University of Gaza Dr. Talal Skaik
  • 2. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Transistor Construction 2 Dr. Talal Skaik 2014 •The npn BJT consists of three semiconductor regions: the emitter region (n type), the base region (p type), and the collector region (n type). •The pnp BJT consists of three semiconductor regions: the emitter region (p type), the base region (n type), and the collector region (p type). There are two types of transistors: • pnp • npn The terminals are labeled: • E - Emitter • B - Base • C - Collector
  • 3. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Transistor Construction 3 Dr. Talal Skaik 2014 The transistor consists of two pn junctions, the emitter–base junction (EBJ) and the collector–base junction (CBJ).
  • 4. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Transistor Construction 4 Dr. Talal Skaik 2014 Emitter: The portion on one side of transistor that supplies charge carriers (i.e. electrons or holes) to the other two portions. The emitter is a heavily doped region. Emitter of PNP transistor supplies hole charges to its junction with the base. Similarly, the emitter of NPN transistor supplies free electrons to its junction with the base.
  • 5. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Transistor Construction 5 Dr. Talal Skaik 2014 Collector is the portion on the other side of the transistor (i.e. the side opposite to the emitter) that collects the charge carriers (i.e. electrons or holes). The doping level of the collector is in between the heavily doping of emitter and the light doping of the base. Base: The middle portion which forms two PN junctions between the emitter and the collector is called the base. The base of transistor is thin, as compared to the emitter and is a lightly doped portion. The function of base is to control the flow of charge carrier.
  • 6. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky BJT Modes Of Operation 6 Dr. Talal Skaik 2014 There are two junctions in bipolar junction transistor. Each junction can be forward or reverse biased independently. Thus there are different modes of operations: Forward Active. Cut off. Saturation.
  • 7. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky BJT Modes Of Operation 7 Dr. Talal Skaik 2014 FORWARD ACTIVE Emitter-base junction is forward biased and collector-base junction is reverse biased. The BJT can be used as an amplifier and in analog circuits. CUTT OFF When both junctions are reverse biased it is called cut off mode. In this situation there is nearly zero current and transistor behaves as an open switch. SATURATION In saturation mode both junctions are forward biased. Large collector current flows with a small voltage across collector base junction. Transistor behaves as an closed switch.
  • 8. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Operation of pnp transistor in active mode 8 Dr. Talal Skaik 2014 Reverse-biased junction of a pnp transistor Forward-biased junction of a pnp transistor.
  • 9. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Operation of pnp transistor in active mode 9 Dr. Talal Skaik 2014 With the external sources, VEE and VCC, connected as shown: • The emitter-base junction is forward biased • The base-collector junction is reverse biased
  • 10. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Currents in a Transistor The collector current is comprised of two currents: B I C I E I   minority CO I majority C I C I   Emitter current is the sum of the collector and base currents: 10 Dr. Talal Skaik 2014 The minority current is called the leakage current and is given by the symbol ICO (IC current with emitter terminal Open).
  • 11. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Common Base Configuration 11 Dr. Talal Skaik 2014 The base is common to both input (emitter–base) and output (collector–base) of the transistor.
  • 12. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Common-Base Configuration Input Characteristics This curve shows the relationship between of input current (IE) to input voltage (VBE) for three output voltage (VCB) levels. 12 Dr. Talal Skaik 2014 VBE=0.7 V
  • 13. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky This graph demonstrates the output current (IC) to an output voltage (VCB) for various levels of input current (IE). Common-Base Configuration Output Characteristics 13 Dr. Talal Skaik 2014
  • 14. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Operating Regions • Active – Operating range of the amplifier. It is noticed that IE is approximately equal to IC (IC≈ IE ). • Cutoff – the region where the collector current is approximately 0A (IC=ICBO). The amplifier is basically off. There is voltage, but little current. • Saturation – Region to the left of VCB=0. Note the exponential increase in collector current as the voltage VCB increases toward 0 V. There is current but little voltage. 14 Dr. Talal Skaik 2014
  • 15. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky E I C I  Silicon) (for V 0.7 BE V  Approximations Emitter and collector currents: Base-emitter voltage: 15 Dr. Talal Skaik 2014
  • 16. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey 07458 • All rights reserved. Electronic Devices and Circuit Theory, 10/e Robert L. Boylestad and Louis Nashelsky Ideally: a = 1 In reality: a is between 0.9 and 0.998 Alpha (a) Alpha (a) is the ratio of IC to IE : E I C I α  dc Alpha (a) in the AC mode: Δ Δ constant ac IC IE VCB α   16 Dr. Talal Skaik 2014 E I CBO I αI C  