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EST 130, Bipolar Junction
Transistors
MEC
2
Contents
• Introduction.
• BJT (Transistor) Types.
• Operating Regions.
• Early Effect.
• Transistor Configurations.
• Transistor Characteristics.
• Comparison.
• Transistor Testing.
3
Transistor Invention
4
Transistor Invention
• First transistor called a point-contact
transistor on December 23, 1947.
• Walter H. Brattain and John Bardeen
demonstrated the amplifying action of first
transistor at Bell Telephone Laboratories.
• Was the predecessor to the junction
transistor invented by Shockley in 1948.
• Shared Nobel Prize in Physics in 1956.
5
6
Bipolar Junction Transistor
• Three terminal device – Emitter, Base and
Collector.
• Two p-n junctions – Emitter-Base junction
and Collector-Base junction.
• PNP and NPN transistors.
• Current controlled – base current controls
the device.
• Can be used in amplifiers or as switches.
• Four regions of operation.
• Three Configurations – Common Emitter,
Common Base and Common Collector.
7
Bipolar Junction Transistor
• Three doped regions.
• Base narrow region
sandwiched between the
larger collector and
emitter regions.
• Emitter region heavily
doped.
• Emitter injects current
carriers into the base.
• Base region very thin
and lightly doped.
Electrons are the majority
carriers in a n type material.
Holes are the majority
carriers in a p type material.
8
Bipolar Junction Transistor
• Most of the current carriers injected into
the base from the emitter pass on to the
collector, do not flow out of the base lead.
• Collector region moderately doped, largest
of all three regions.
• Collector region attracts carriers injected
into the base region.
• Collector region the largest region, must
dissipate more heat than emitter or base
regions.
9
Doping in Transistor Structures
Emitter
Heavily
Doped
Base
Lightly
Doped
Collector
Moderately
Doped
e
b
c
Thin Largest
Two types of carriers – holes and electrons, hence bipolar.
10
Depletion Regions
(Unbiased)
• Diffusion of electrons
from both n regions
into the p -type base
causes a barrier
potential for both p-n
junctions.
• e-b depletion region
narrower than the c-b
depletion region due
to difference in doping
levels.
Barrier Potential = 0.7 V
11
Depletion Regions
(Unbiased)
• Heavy doping in the emitter region.
• Penetration into the n material minimal
due to the availability of many free
electrons.
• Fewer free electrons due to moderate
doping level in the collector region.
• Depletion layer penetrate deeper into the
collector region.
12
Bipolar Junction Transistors
Can two back to back connected pn
junction diodes function as a npn
transistor?
Base width higher?
Recombination
in the base?
13
Bipolar Junction Transistors
• Two back-to-back pn diodes can't function
as a single BJT.
• Transistor operation not achieved with
standalone pn diodes which conduct a
negligible currents under reverse bias.
• Excess electrons from the p side of the
forward biased diode can not be swept to
the p side of the reverse biased diode
through the metal wire in a "BJT like diode
configuration".
14
Bipolar Junction Transistors
• Excess electrons from the p side of the
forward biased diode are swept to the
power supply (stronger pull) providing a
voltage bias to the common terminal of the
diodes.
• For transistor functionality, semiconductor
only thin lightly doped Base region
required.
• With a metal introduced in the path (two
back-to-back diodes), no BJT functionality
possible.
15
Transistor Operating Regions
Operating
Region
Emitter –
Base
Junction
Collector –
Base
Junction
Applications
Active
Region
Forward
Biased
Reverse
Biased
Amplifiers
Saturation
Region
Forward
Biased
Forward
Biased Switches
(on/off)
Cut off
Region
Reverse
Biased
Reverse
Biased
Inverse Active
Region
Reverse
Biased
Forward
Biased
-
16
Transistor Currents
• For a transistor amplifier, emitter-base
junction forward-biased, and collector-
base junction reverse-biased.
• Common connection for voltage sources
at the base lead.
• Electrons in the n -type emitter repelled
into the base by the negative terminal of
the emitter supply voltage.
17
Transistor Currents
• Base is very thin and lightly doped.
• Only a few electrons combine with holes in
the base.
• Small current flowing out of the base lead
called recombination current.
• Free electrons injected into the base must
fall into a hole before they can flow out the
base lead.
18
Transistor Currents
• Most of the emitter-injected electrons pass
through the base region to the collector
region.
• A small voltage creates a strong electric
field in the collector-base junction to attract
almost all free electrons injected into the
base.
• Positive collector-base voltage attracts
free electrons in the p - type base to the
collector side before they recombine with
holes in the base.
19
Early Effect/Base Width
Modulation
• As reverse bias across the collector-base
junction increases, depletion region
penetrates more into the base.
• Thin base lightly doped, penetration into
the base region larger than into the
collector, effective base width decreases/
modulated.
• Punch through – large reverse bias,
depletion region penetrates the entire
base, transistor action lost, large current
flow damage.
20
Transistor Configurations
21
Common Base Configuration
• Collector current nearly identical to the
emitter current.
IC ≈ IE
RC, RE for Current Limiting.
RC
RE
RC
RE
Common Base Configuration
Base is Common
22
Common Base Current Gain
• dc alpha (αdc) describes how closely the
emitter and collector currents are in a
common base circuit.
• In most cases, the dc alpha 0.99 or
greater.
• The thinner and more lightly doped the
base, the closer the value of alpha to one.
23
Circuit for Common Base
Characteristics
Input Side Output Side
24
Common Base Characteristics
Input Characteristics Output Characteristics
25
Common Emitter Configuration
Emitter common to input and output.
@ 25oC
Phase Inversion.
26
Common Emitter Current Gain
• dc current gain of a transistor in common-
emitter connection called dc beta.
• Again,
• Or,
DC Equivalent of a Transistor
27
Circuit for Common Emitter
Characteristics
28
Common Emitter Input
Characteristics
29
Common Emitter Output
Characteristics
Active Region
Saturation Region
Cut Off
Region
CE
ac
C
V
r
I



C
ac
B
I
I




30
Common Emitter Amplifier
RC Coupled Amplifier
Voltage Divider Bias
Coupling Capacitor
For Current Limiting
31
Transistor Switch
32
CB and CE Parameters
33
Common Collector Configuration
Collector common to
input and output
Emitter Follower.
No phase inversion for the
output.
For Impedance Matching.
Voltage Gain ≈ 1.
Used in cascade amplifiers.
34
Common Collector Current Gain
• Common Collector Current Gain:
• Again
and
E
dc
B
I
I
 
1
dc dc
 
 
1
1
dc
dc




35
Circuit for Common Collector
Characteristics
36
Common Collector Characteristics
37
Voltage Follower Circuit
38
Brief Comparison
Characteristic CB CE CC
Input Resistance Low Medium High
Output Resistance Very
High
High Low
Voltage Gain High Medium Low
Current Gain Low Medium High
39
Darlington Pair
Current Gain Improves
β1
β2
βd = β1.β2
40
Cascode Configuration
41
42
Transistor Testing
• Identify whether pnp or npn.
• Identify transistor leads.
• Use of Ohmmeter/Multimeter.
• Consider the transistor as two diodes.
• Emitter-base and collector-base junctions
forward biased – low resistance.
• Emitter-base and collector-base junctions
reverse biased – high resistance.
• Emitter to collector – high resistance.
43
Transistor Testing
44
Thank You

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EST 130, Bipolar Junction Transistors

  • 1. 1 EST 130, Bipolar Junction Transistors MEC
  • 2. 2 Contents • Introduction. • BJT (Transistor) Types. • Operating Regions. • Early Effect. • Transistor Configurations. • Transistor Characteristics. • Comparison. • Transistor Testing.
  • 4. 4 Transistor Invention • First transistor called a point-contact transistor on December 23, 1947. • Walter H. Brattain and John Bardeen demonstrated the amplifying action of first transistor at Bell Telephone Laboratories. • Was the predecessor to the junction transistor invented by Shockley in 1948. • Shared Nobel Prize in Physics in 1956.
  • 5. 5
  • 6. 6 Bipolar Junction Transistor • Three terminal device – Emitter, Base and Collector. • Two p-n junctions – Emitter-Base junction and Collector-Base junction. • PNP and NPN transistors. • Current controlled – base current controls the device. • Can be used in amplifiers or as switches. • Four regions of operation. • Three Configurations – Common Emitter, Common Base and Common Collector.
  • 7. 7 Bipolar Junction Transistor • Three doped regions. • Base narrow region sandwiched between the larger collector and emitter regions. • Emitter region heavily doped. • Emitter injects current carriers into the base. • Base region very thin and lightly doped. Electrons are the majority carriers in a n type material. Holes are the majority carriers in a p type material.
  • 8. 8 Bipolar Junction Transistor • Most of the current carriers injected into the base from the emitter pass on to the collector, do not flow out of the base lead. • Collector region moderately doped, largest of all three regions. • Collector region attracts carriers injected into the base region. • Collector region the largest region, must dissipate more heat than emitter or base regions.
  • 9. 9 Doping in Transistor Structures Emitter Heavily Doped Base Lightly Doped Collector Moderately Doped e b c Thin Largest Two types of carriers – holes and electrons, hence bipolar.
  • 10. 10 Depletion Regions (Unbiased) • Diffusion of electrons from both n regions into the p -type base causes a barrier potential for both p-n junctions. • e-b depletion region narrower than the c-b depletion region due to difference in doping levels. Barrier Potential = 0.7 V
  • 11. 11 Depletion Regions (Unbiased) • Heavy doping in the emitter region. • Penetration into the n material minimal due to the availability of many free electrons. • Fewer free electrons due to moderate doping level in the collector region. • Depletion layer penetrate deeper into the collector region.
  • 12. 12 Bipolar Junction Transistors Can two back to back connected pn junction diodes function as a npn transistor? Base width higher? Recombination in the base?
  • 13. 13 Bipolar Junction Transistors • Two back-to-back pn diodes can't function as a single BJT. • Transistor operation not achieved with standalone pn diodes which conduct a negligible currents under reverse bias. • Excess electrons from the p side of the forward biased diode can not be swept to the p side of the reverse biased diode through the metal wire in a "BJT like diode configuration".
  • 14. 14 Bipolar Junction Transistors • Excess electrons from the p side of the forward biased diode are swept to the power supply (stronger pull) providing a voltage bias to the common terminal of the diodes. • For transistor functionality, semiconductor only thin lightly doped Base region required. • With a metal introduced in the path (two back-to-back diodes), no BJT functionality possible.
  • 15. 15 Transistor Operating Regions Operating Region Emitter – Base Junction Collector – Base Junction Applications Active Region Forward Biased Reverse Biased Amplifiers Saturation Region Forward Biased Forward Biased Switches (on/off) Cut off Region Reverse Biased Reverse Biased Inverse Active Region Reverse Biased Forward Biased -
  • 16. 16 Transistor Currents • For a transistor amplifier, emitter-base junction forward-biased, and collector- base junction reverse-biased. • Common connection for voltage sources at the base lead. • Electrons in the n -type emitter repelled into the base by the negative terminal of the emitter supply voltage.
  • 17. 17 Transistor Currents • Base is very thin and lightly doped. • Only a few electrons combine with holes in the base. • Small current flowing out of the base lead called recombination current. • Free electrons injected into the base must fall into a hole before they can flow out the base lead.
  • 18. 18 Transistor Currents • Most of the emitter-injected electrons pass through the base region to the collector region. • A small voltage creates a strong electric field in the collector-base junction to attract almost all free electrons injected into the base. • Positive collector-base voltage attracts free electrons in the p - type base to the collector side before they recombine with holes in the base.
  • 19. 19 Early Effect/Base Width Modulation • As reverse bias across the collector-base junction increases, depletion region penetrates more into the base. • Thin base lightly doped, penetration into the base region larger than into the collector, effective base width decreases/ modulated. • Punch through – large reverse bias, depletion region penetrates the entire base, transistor action lost, large current flow damage.
  • 21. 21 Common Base Configuration • Collector current nearly identical to the emitter current. IC ≈ IE RC, RE for Current Limiting. RC RE RC RE Common Base Configuration Base is Common
  • 22. 22 Common Base Current Gain • dc alpha (αdc) describes how closely the emitter and collector currents are in a common base circuit. • In most cases, the dc alpha 0.99 or greater. • The thinner and more lightly doped the base, the closer the value of alpha to one.
  • 23. 23 Circuit for Common Base Characteristics Input Side Output Side
  • 24. 24 Common Base Characteristics Input Characteristics Output Characteristics
  • 25. 25 Common Emitter Configuration Emitter common to input and output. @ 25oC Phase Inversion.
  • 26. 26 Common Emitter Current Gain • dc current gain of a transistor in common- emitter connection called dc beta. • Again, • Or, DC Equivalent of a Transistor
  • 27. 27 Circuit for Common Emitter Characteristics
  • 29. 29 Common Emitter Output Characteristics Active Region Saturation Region Cut Off Region CE ac C V r I    C ac B I I    
  • 30. 30 Common Emitter Amplifier RC Coupled Amplifier Voltage Divider Bias Coupling Capacitor For Current Limiting
  • 32. 32 CB and CE Parameters
  • 33. 33 Common Collector Configuration Collector common to input and output Emitter Follower. No phase inversion for the output. For Impedance Matching. Voltage Gain ≈ 1. Used in cascade amplifiers.
  • 34. 34 Common Collector Current Gain • Common Collector Current Gain: • Again and E dc B I I   1 dc dc     1 1 dc dc    
  • 35. 35 Circuit for Common Collector Characteristics
  • 38. 38 Brief Comparison Characteristic CB CE CC Input Resistance Low Medium High Output Resistance Very High High Low Voltage Gain High Medium Low Current Gain Low Medium High
  • 39. 39 Darlington Pair Current Gain Improves β1 β2 βd = β1.β2
  • 41. 41
  • 42. 42 Transistor Testing • Identify whether pnp or npn. • Identify transistor leads. • Use of Ohmmeter/Multimeter. • Consider the transistor as two diodes. • Emitter-base and collector-base junctions forward biased – low resistance. • Emitter-base and collector-base junctions reverse biased – high resistance. • Emitter to collector – high resistance.