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Operation Theory BIPOLAR JUNCTION TRANSISTOR (BJT) Engr.Usman Ali khan

Bipolar Junction Transistor (BJT)

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Bipolar Junction Transistor (BJT). Operation Theory. Engr.Usman Ali khan. Contents. BJT Formation BJT Terminals Biasing of BJT BJT Currents α of BJT. Formation of BJT. N. P. N. P. N. P. Two Junctions. Two Junctions. - PowerPoint PPT Presentation

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Page 1: Bipolar Junction Transistor (BJT)

Operation Theory

BIPOLAR JUNCTION TRANSISTOR (BJT)

Engr.Usman Ali khan

Page 2: Bipolar Junction Transistor (BJT)

CONTENTS

1. BJT Formation

2. BJT Terminals

3. Biasing of BJT

4. BJT Currents

5. α of BJT

Page 3: Bipolar Junction Transistor (BJT)

FORMATION OF BJT

P N P

Two Junctions

N P N

Two Junctions

N-Type material has excessive free electrons and P-Type material has excessive holes

NPN and PNP BJTs have same characteristics. The only difference is in their polarities of applied voltages. The polarities are reversed for the two types of transistor.

Page 4: Bipolar Junction Transistor (BJT)

BJT TERMINALS

N P N

Emitter Collector

Base

N NPE C

B

Base-Emitter Junction Base-Collector Junction

Page 5: Bipolar Junction Transistor (BJT)

BJT CIRCUIT SYMBOLS

N NPE C

B B

CE

C

E

B

P PNE C

B B

CE

C

E

B

Page 6: Bipolar Junction Transistor (BJT)

FORWARD BIASED JUNCTION OPERATION

+

+

+

-

-

-

E

NP

+ -

Opposing field due to battery

Electrons Push electrons to the other side

Positive terminal attracts electrons

Flow of electron current; but in semiconductor electronics the flow of positive or conventional current is considered

Page 7: Bipolar Junction Transistor (BJT)

REVERSE BIASED JUNCTION OPERATION

+

+

+

-

-

-

E

NP

+-

Supporting field due to battery Electrons Push Minority Carrier electrons to the other side

Positive terminal attracts Minority Carrier electrons

Current flows due to minority carriers

Page 8: Bipolar Junction Transistor (BJT)

BJT BIASING

N P N

Emitter Collector

Base- +

- +

VEE VCC

- +

+-

ON

OFF

Page 9: Bipolar Junction Transistor (BJT)

BJT CURRENTS

N P N

Emitter Collector

Base- +

- +

VEE VCC

Negative Terminal pushes electrons to the other side

When electrons come to Base, they become minority carriers

Minority carriers are attracted to the positive terminal of the battery

Some electrons escape to the ground

Page 10: Bipolar Junction Transistor (BJT)

BJT CURRENTS

N NP

EC

B

Conventional Current

Electron Current

-+

IB

IE IC (INJ)

IE = IB + IC(INJ)

Page 11: Bipolar Junction Transistor (BJT)

COLLECTOR-BASE REVERSE CURRENT

N NP

EC

B

ICBO

Conventional Current

Electron Current

When Collector-Base Junction is reverse biased and Emitter-Base Junction is Open, a reverse current flows in this reverse biased junction which is called ICBO

Total Collector current is = IC = IC(INJ) + ICBO

Page 12: Bipolar Junction Transistor (BJT)

Α OF BJT

α = IC(INJ)/IE

IC = IC(INJ) + ICBO ICBO<<IC(INJ)

IC = IC(INJ)

α = IC/IE

Page 13: Bipolar Junction Transistor (BJT)

HOME WORK• Example: 4.1

• End Problems: 4.1 4.5