Bipolar Junction Transistors
description
Transcript of Bipolar Junction Transistors
![Page 1: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/1.jpg)
BB
CC
EE
![Page 2: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/2.jpg)
Transistors
• They are unidirectional current carrying devices like diodes with capability to control the current flowing through them
• Bipolar Junction Transistors (BJT) control current by current
• Field Effect Transistors (FET) control current by voltage
• They can be used either as switches or as amplifiers
![Page 3: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/3.jpg)
• A transistor allows you to control the current, not just block it in one direction.
• A good analogy for a transistor is a pipe with an adjustable gate.
• A transistor has three terminals.
• The main path for current is between the collector and emitter.
• The base controls how much current flows, just like the gate controls the flow of water in the pipe.
![Page 4: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/4.jpg)
BIPOLAR JUNCTION TRANSISTOR
• Two back to back P-N junctions• Emitter
– Heavily doped– Main function is to supply majority carriers to base
• Base– Lightly doped as compared to emitter– Thickness 10-6 m
• Collector– Collect majority carriers from emitter through base– Physically larger than the emitter region
EE
BB
NN PP NN CC EE
BB
PP NN PP CC
![Page 5: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/5.jpg)
The BJT – Bipolar Junction TransistorThe BJT – Bipolar Junction Transistor
The Two Types of BJT TransistorsThe Two Types of BJT Transistors
npnnpn pnppnp
nn pp nnEE
BB
CC pp nn ppEE
BB
CC
Cross SectionCross Section Cross SectionCross Section
BB
CC
EE
Schematic Schematic SymbolSymbol
BB
CC
EE
Schematic Schematic SymbolSymbol
![Page 6: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/6.jpg)
LP4 6
NPN Bipolar Junction Transistor
![Page 7: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/7.jpg)
LP4 7
PNP Bipolar Junction Transistor
![Page 8: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/8.jpg)
• The collector surrounds the emitter region, making it almost impossible for the electrons injected into the base region to escape being collected, thus making the resulting value of α very close to unity, and so, giving the transistor a large β
STRUCTURE
![Page 9: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/9.jpg)
• Energy Band diagram of an unbiased transistor– N-region moves down and P-region moves up due to
diffusion of majority carriers across junction.– The displacement of band and carrier migration
stops when Fermi levels in the three regions are equalized
Biasing of Transistor– Base and emitter current when collector is open
• EB is forward biased- electron diffusion from emitter to base and hole diffusion from base to emitter
• Hence IB will be large and is equal to IE
• Collector is open so no current flows into collector
![Page 10: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/10.jpg)
• Base and Collector current when the Emitter is open (ICBO)
• CB is reverse biased- electron from base flow into collector region and holes from collector flow into base
• This current is known as reverse saturation current
• The base current IB will be small and is equal to ICBO
![Page 11: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/11.jpg)
• Four Ways of Transistor biasing– Both EB and CB junctions are fwd biased- Huge
current flows through base. The transistor is said to be operating in Saturation region (mode)
– Both EB and CB junctions are reverse biased- The transistor is said to be operating in cut off region (mode)
– EB junction is fwd biased and CB junction is reverse biased. The collector current is controlled by emitter current or base current- The transistor is said to operate in Active region (mode)
– EB junction in reverse biased and CB junction in fwd biased- inverted region (mode)
![Page 12: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/12.jpg)
Transistor Biasing-Active RegionWhen both Emitter and Collector are closed
• Emitter-base junction is forward biased• Collector-base junction is reverse biased
• DC emitter supply voltage (VEE)- Negative terminal of VEE is connected to emitter
• DC collector supply voltage (VCC)- Positive terminal of VCC is connected to collector
• IB becomes very small and IC will be as large as IE
NN PP NN
VVEEEE VVCCCC
IIEE IICC
IIBB
![Page 13: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/13.jpg)
Transistor currents• Forward biasing from base to emitter narrows the BE
depletion region• Reverse biasing from base to collector widens the
depletion CB region• Conduction electrons diffuse into p-type base region• Base is lightly doped and also very thin- so very few
electron combine with available hole and flow out of the base as valence electrons (small base electron current)
N P N
VEE VCC
IE IC
IB
![Page 14: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/14.jpg)
• Sufficient holes are not avail in base – remote possibility of joining of electrons with holes
• Electron concentration is large on emitter side and nil on collector
• Electrons swiftly move towards collector• At CB junction they are acted upon by strong electric
field due to reverse bias and are swept into collector
![Page 15: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/15.jpg)
Transistor currents• Most of the electrons diffuse into CB depletion region
• These electrons are pulled across the reverse biased CB junction by the attraction of the collector supply voltage and form the collector electron current. Therefore
IE= IC + IB
• 1-2% of emitter current goes to supply base current and 98-99% goes to supply collector current
• Moreover, IE flows into the transistor and IB & IC flow out of transistor
• Current flowing in is taken as positive and currents flowing out are taken as negative
• The ratio of the number of electrons arriving at collector to the number of electrons emitted by the emitter is called base transportation factor
![Page 16: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/16.jpg)
Important Biasing Rule• Both collector and base are positive with respect to
emitter• But collector is more positive than base• Different potentials have been designated by double
subscripts as shown in the figure
• VCB (Collector is more positive than base) and VBE (base is more positive than emitter)
++ C
- E
+B
VCB
VBE
E C
+B
- ++
VBE VCB
![Page 17: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/17.jpg)
Transistor circuit configuration• There are of three types
– Common base (CB) OR grounded base– Common emitter (CE) OR grounded emitter– Common collector (CC) OR grounded collector
• Common is the term used to denote the electrode that is common to the input and output circuits and it is generally grounded
• Common-Base Biasing (CB) : input = VBE & IE
• output = VCB & IC
• Common-Emitter Biasing (CE): input = VBE & IB
• output = VCE & IC
• Common-Collector Biasing (CC): input = VBC & IB
• output = VEC & IE
![Page 18: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/18.jpg)
Common Base Configuration• Input signal applied between emitter & base• Output is taken from collector & base• Ratio of collector current to emitter current
is called dc alpha (dc) of a transistor
E C
+
B
- ++
VBE VCB
![Page 19: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/19.jpg)
• The subscript dc on signifies that this ratio is defined from dc values of IC and IE
• There is also an ac which refers to the ratio of change in collector current to the change in emitter current
• For all practical purposes dc= ac=
• IE is taken as positive (flowing into transistor) and IC is taken as negative (flowing out of transistor)
• is the measure of quality of a transistor- higher its values, better is the transistor
• Value ranges from 0.95 to 0.999
EdcC
E
Cdc
II
OR
I
I
![Page 20: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/20.jpg)
Common Emitter Configuration• The input signal is applied between the base and emitter
and the output signal is taken out from the collector and the emitter
• Ratio of collector current to base current is called dc beta (dc) of a transistor
C
E
+B
-
BC
B
C
II
OR
I
I
Relation between and
E
C
I
I
B
C
I
Iand
![Page 21: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/21.jpg)
B
E
I
I
CEB III usingB
C
I
Ithen becomes
CE
C
II
I
or
1//
/
ECEE
EC
IIII
II
1 or 1 or 1/
Common Collector Configuration• The input signal is applied between the base and
collector and the output signal is taken out from the emitter-collector circuit
• Ratio of emitter current to base current is
11/
.B
C
C
E
B
E
I
I
I
I
I
I
![Page 22: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/22.jpg)
From the figureC
E
+B- BBBCBE IIIIII 1
Output current=(1+) x Input current
Relation between transistor currents
CBE III ::We know
EBC III and
EEEEC
B IIIII
I
11
1/
1
1
and
because
1
11We get
![Page 23: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/23.jpg)
• This shows that emitter current initiated by the forward biased emitter base junction is split into two parts
• (1-)IE which becomes base current in the external circuit
IE which becomes collector current in the external circuit
Therefore
:)1(:1
:)1(:
EEE III
![Page 24: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/24.jpg)
![Page 25: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/25.jpg)
Static Characteristics• Common Base Static characteristics
–Input characteristics. IE varies with VBE when voltage VCB is held constant
• VCB is adjusted with the help of R1
• VBE is increased and corresponding values of IE are noted
• The plot gives input characteristics• Similar to the forward characteristics of P-N diode• This characteristics is used to find the input
resistance of the transistor. Its value is given by the reciprocal of its slope
Rin= VBE / IE
![Page 26: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/26.jpg)
BJT Input CharacteristicsBJT Input Characteristics
VVBEBE
IIEE
2 2 mAmA
4 4 mAmA
6 6 mAmA
8 8 mAmA
0.7 V0.7 V
VCC
E C
+
B
VBE
VCB
ICIE
VEE
R1R2
![Page 27: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/27.jpg)
Static Characteristics• Common Base Static characteristics
– Output characteristics. IC varies with VCB when IE is held constant
• VBE is adjusted with the help of R2 and IE is held constant
• VCB is increased and corresponding values of IC are noted
• The plot gives output characteristics
• Then IE is increased to a value little higher and whole process is repeated
• The output resistance of the transistor is given by
Rout= VCB / IC
VCC
E C
+
B
VBEVCB
ICIE
VEE
R1R2
![Page 28: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/28.jpg)
IICC flows even when V flows even when VCBCB=0 for different values of =0 for different values of
IIEE(due to internal junction voltage at CB junction)(due to internal junction voltage at CB junction)
IICC flows even when I flows even when IEE=0 (Collector leakage current or =0 (Collector leakage current or
reverse saturation current Ireverse saturation current ICBOCBO))
The output resistance is very high (500k)
Sa
tura
tio
n R
egio
nS
atu
rati
on
Reg
ion
IIEE
IICC
VVCBCB
Active Active RegionRegion
CutoffCutoff
IIEE = 0 = 0
BJT Output CharacteristicsBJT Output Characteristics
![Page 29: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/29.jpg)
Static Characteristics– It can be seen that IC flows even when VCB is zero
– It is due to the fact that electrons are being injected into base due to forward biased E-B junction and are collected by collector due to action of internal junction voltage at C-B junction
– Another important feature is that a small amount of collector current flows even when the emitter current IE
is zero called collector leakage current (IICBOCBO)
– When VCB is permitted to increase beyond a certain value, IC increases rapidly due to avalanche breakdown
• This characteristics may be used to find ac
ac =IC/ IE
![Page 30: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/30.jpg)
LP4 30Common Emitter(CE) Connection
Common Emitter Configuration• Transistor is biased in active region• Called CE because emitter is common to both VBB and VCC• VBB forward biases the EB junction and VCC reverse biases the CB
VCC
BC
B
E
VBE
VCE
ICIB
VBB
R1R2
![Page 31: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/31.jpg)
Static Characteristics
• Common Emitter Static characteristics– Input characteristics. IB varies with VBE when
voltage VCE is held constant
• VCE is adjusted with the help of R1
• VBE is increased and corresponding values of IB are noted
• The plot gives input characteristics
• Procedure is repeated for different (constant) values of VCE
• This characteristics is used to find the input resistance of the transistor. Its value is given by the reciprocal of its slope
Rin= VBE / IB
![Page 32: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/32.jpg)
VVBEBE
IIBB
2 mA2 mA
4 mA4 mA
6 mA6 mA
8 mA8 mA
0.7 V0.7 V
![Page 33: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/33.jpg)
Static Characteristics• Common Emitter Static characteristics
– Output characteristics. IC varies with VCE when IB is held constant
• IB is held constant
• VCE is increased and corresponding values of IC are noted
• The plot gives output characteristics
• Then IB is increased to a value little higher and whole process is repeated
• The output resistance in this case is very less as compared to CB circuit and is given by
Rout= VCE / IC
![Page 34: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/34.jpg)
As VAs VCECE increases from zero, I increases from zero, ICC rapidly increases to saturation level for a fixed rapidly increases to saturation level for a fixed
value of Ivalue of IBB
IICC flows even when I flows even when IBB=0 (Collector leakage current or reverse saturation =0 (Collector leakage current or reverse saturation
current Icurrent ICEOCEO), the transistor is said to be cutoff), the transistor is said to be cutoff
When VCB is permitted to increase beyond a certain value, IC increases rapidly due to avalanche breakdown
This characteristics may be used to find ac ac =IC/ IB
VVCECE
IICC
Active Active RegionRegion
IIBB
Saturation RegionSaturation RegionCutoff RegionCutoff Region
IIBB = 0 = 0
Region of Operation
Description
Active Small base current controls a large collector current
Saturation VCE(sat) ~ 0.2V, VCE increases with IC
Cutoff Achieved by reducing IB to 0, Ideally, IC will also equal 0.
![Page 35: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/35.jpg)
BCE III
EdcCE
Cdc II
I
I
CBOCE III ,0where
Therefore, in general CBOEdcC III
Common Base
Common Emitter
BCE III
BdcCB
Cdc II
I
I
(Reverse saturation current)
![Page 36: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/36.jpg)
1
where CEOCB III ,0
CEOBdcC III
(Reverse saturation current)
Relationship between dc and dc
1
and
![Page 37: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/37.jpg)
Common Base Formulas
VCC
E C
B
VBE
VCB
ICIE
IB
VEE
RLRE
E
BEEEEBEEEEE R
VVIVRIV
0
Where VBE=0.3 V for Ge and 0.7 V for Si
Generally VEE>>VBE so IE=VEE/RE
LCCCCBCBLCCC RIVVVRIV 0
and
![Page 38: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/38.jpg)
Common Emitter Formulas
B
BEBBEBEBBBB R
VVIVRIV
0
LCCCCECELCCC RIVVVRIV 0
and
VCC
E C
B
VBE
VCE
ICIB
IE
VBB
RLRB
![Page 39: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/39.jpg)
DC DC and DC and DC
= Common-emitter current gain= Common-emitter current gain
= Common-base current gain= Common-base current gain
= I= ICC = I = ICC
IIBB I IEE
The relationships between the two parameters are:The relationships between the two parameters are:
= = = =
+ 1+ 1 1 - 1 -
Note: Note: and and are sometimes referred to as are sometimes referred to as dcdc and and dcdc
because the relationships being dealt with in the BJT because the relationships being dealt with in the BJT are DC.are DC.
![Page 40: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/40.jpg)
BJT ExampleBJT ExampleUsing Common-Base NPN Circuit ConfigurationUsing Common-Base NPN Circuit Configuration
++__
++__
Given: IGiven: IBB = 50 = 50 A , I A , ICC = 1 mA = 1 mA
Find: IFind: IEE , , , and , and
Solution:Solution:
IIEE = I = IBB + I + ICC = 0.05 mA + 1 mA = 1.05 mA = 0.05 mA + 1 mA = 1.05 mA
= I= ICC / I / IBB = 1 mA / 0.05 mA = 20 = 1 mA / 0.05 mA = 20
= I= ICC / I / IEE = 1 mA / 1.05 mA = 0.95238 = 1 mA / 1.05 mA = 0.95238
could also be calculated using the value of could also be calculated using the value of with the formula from the previous slide. with the formula from the previous slide.
= = = 20 = 0.95238 = 20 = 0.95238
+ 1 21+ 1 21
IICC
IIEE
IIBB
VVCBCB
VVBEBE
EE
CC
BB
![Page 41: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/41.jpg)
Transistor as an amplifier
![Page 42: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/42.jpg)
Transistor as an amplifier• An electronic circuit that causes an increase in the
voltage or power level of a signal• It is defined as the ratio of the output signal voltage to
the input signal voltage
i
o
v
v
geInputVolta
ageOutputVoltG
VVEEEE VVCCCC
IIEE IICC
IIBB RRLL
![Page 43: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/43.jpg)
i
iE r
vI
In the figure we see that an output voltage is developed across RL
The dc voltage VEE is a fixed voltage and causes a dc current IE to flow through EB junction
When the ac voltage Vi is super-imposed on VEE, the emitter base voltage varies with time
Say if VEE =10V and the peak voltage of Vi is is 1V, the EB voltage swings from 9V to 11V
The causes corresponding variations in IE and IC which gives Vo
The emitter variation due to EB voltage variation can be expressed as
![Page 44: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/44.jpg)
The collector current IC changes by
EdcC II This current IC flows through RL causing a voltage drop
Liidco
LEdco
LCo
Rrvv
RIv
RIv
/
iLdcio rRvvG //
Hence
as 1dc
Where ri is very small (100 ) and RL is of the order of kilo-ohms. It means Vo is larger than Vi indicating that the transistor has amplified small Vi to a larger Vo
![Page 45: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/45.jpg)
Problems• In the CE Transistor circuit VBB= 5V, RBB=
107.5 k, RCC = 1 k, VCC = 10V. Find IB, IC, VCE, and the transistor power dissipation
![Page 46: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/46.jpg)
BB
BEBBB R
VVI
In the CE Transistor circuit shown earlier VBB= 5V, RBB= 107.5 k, RCC = 1 k, VCC = 10V. Find IB, IC, VCE, and the transistor power dissipation using the characteristics as shown belowBy Applying KVL to the base emitter circuit
By using this equation along with the iB / vBE characteristics of the base
emitter junction, IB = 40 A
By Applying KVL to the collector emitter circuit
CC
CECCC R
VVI
By using this equation along with the iC / vCE characteristics
of the base collector junction, iC = 4 mA, VCE = 6V
![Page 47: Bipolar Junction Transistors](https://reader035.fdocuments.us/reader035/viewer/2022081419/568158ce550346895dc61a19/html5/thumbnails/47.jpg)
10040
4
A
mA
I
I
B
C
Transistor power dissipation = VCEIC = 24 mW
We can also solve the problem without using the characteristics
if and VBE values are known
iB
100 A
0
5V vBE
Input Characteristics Output Characteristics
iC
10 mA
0
vCE
100 A
80 A
60 A
40 A
20 A