2. Classification of Transistor
Two types of transistor as
Unipolar junction transistor
Current conduction due to only majority carrier. Commonly known as
FET. It is voltage operated devices
FET can classified as
Junction Field Effect Transistor (JFET)
Metal Oxide Semiconductor FET (MOSFET)
Metal semiconductor FET (MESFET)
Biploar junction transistor
Current conduction due to both holes and electrons. It is current
operated devices and classified as npn, pnp
4. TRANSISTOR (BJT)
Transistor construction
Types as n-p-n and p-n-p transistor
Three region as
Emitter (E)
Base (B)
Collector (C)
Emitter
It placed one side, which supplies charge carrier to other
region. It is heavily doped
Base
It is middle in region forms two PN junction. It is lightly
doped and thinner region
Collector
It is opposite to the emitter and collect charge. It is larger
region compared to other two. Doping level is intermediate.
5. Standard transistor symbol
It has two junction like two diode
JE as emitter diode and act as F.B
JC as collector diode and act as R.B
6. Modes of operation
If transistor operate as an amplifier, it biased with
external voltages.
Depends on external bias voltage polarity, transistor
works as any one of the three region
7. Transistor operation
E-B junction as F.B and C-B junction as R.B.
Ie flows through the collector region.
Working as npn transistor:
E-B junction as F.B and C-B junction as R.B
Electrons in n-region(E) flows in to p-region(B)
B- lightly doping so that small electrons only recombine to
holes and remaining current flows to n-region (C)
IE=IB+IC
IC has minority carrier and majority carrier current
8. Working as pnp transistor:
E-B junction as F.B and C-B junction as R.B
Holes in p-region(E) flows in to n-region(B)
B- lightly doping so that small holes only recombine to
electrons and remaining holes current flows to p-region
(C)
Current conduction takes place only by holes
But external wiring still current be electron.
9. Types of configuration
Connection of transistor circuit as
One terminal is i/p
Other terminal is o/p
Other terminal common between i/p and o/p
S.No Configuration Input Output Common
terminal
Also Called as
1 CB E C B Grounded Base
Configuration
2 CE B C E Grounded Emitter
Configuration
3 CC B E C Grounded
Collector
Configuration
11. Current amplification factor (α):
Ratio of o/p current to i/p current is nothing but α.
α< unity. α↑ by IB↓. Α range as 0.9 to 0.99
Expression for collector current:
Total collector current consist of
Part of IE reaches to C terminal (αIE)
Ileakage due to minority carrier in B-C jn on account of R.B
Ileakage =ICBO (C-B current with E open)
12. Common Base Characteristics
I/p characteristics
It relates as i/p current (IE) with i/p voltage (VBE) for varies
output voltage (VCB)
13. Observation as
Point 1
IE ↑ rapidly after cut in voltage with small ↑VBE
Indicate Rin is small.
Dynamic i/p resistance as
Point 2
↑VCB then slight ↑IE
Reason as VCB ↑, then width of depletion region (Jc
junction) changed under R.B condition.
Depletion width in Je junction small due to F.B
14. O/p Characteristics
It relates as o/p current (IC) with o/p voltage (VCB) for varies
input current (IE). In diagram Y-axis as IC (wrong)
15. Observation as
Active region
IC ↑ with equal to IE. IC independent on VCB
Relationship as
B-E jn as F.B and C-B jn as R.B
Cut-off region
IE=0, IC=ICBO due to reverse saturation current.
ICBO as on order of μA or nA. Here IC≈0
B-E jn and C-B jn both as R.B
16. Saturation region
This is the region as left of VCB=0
B-E jn and C-B jn both as F.B
Early effect or base width modulation
VC ↑, R.B ↑, then (depletion width between C-B)↑
As result in base width ↓
Causes of base width ↓ as
Less chances of recombination in B- region, then α ↑ with VCB ↑
Charge gradient ↑ in B-region, minority carrier I injected in E-region ↑
Large VC, B-width ↓ effectively (may be zero), causes B.D voltage in
transistor. This phenomenon called punch through.
17. Transistor parameters
Slope of CB char gives different parameter. Which is
nothing but h-parameter.
i/p impedance
Typical value as 20Ω to 50Ω
O/p admittance
Typical value as 0.1μΩ to 10μΩ
Forward current gain
Typical value as 0.9 to 1.0
Reverse voltage gain
Typical value as 10^-5 to 10^-4
19. Base current amplification factor (β):
Ratio of change in o/p current to change in input current.
Relationship between α and β
If α=1 then β=Ꚙ
Conclusion:
Β of CE config is high and so
95% used in this transistor
Configuration.
21. Common Emitter Characteristics
I/p characteristics
Relates i/p current (IB) to i/p voltage (VBE) for varies level
of o/p voltage (VCE) (here Y-axis is IB)
22. Observation as
Point 1
IB ↑ rapidly after cut-in voltage of VBE.
So Rin is small.
Point 2
VCE ↑, IB ↓, here VBE=const
Reason of IB ↓ as R.B ↑ at Jc junction which means C-B
junction.
Then depletion layer width ↑
Width of B-region ↓ and ↓ of recombination in B-region
23. O/p Characteristics
It relates as o/p current (IC) with o/p voltage (VCE) for varies
input current (IB).
24. Observation as
Active region
B-E as F.B and C-B as R.B
VCE ↑, then R.B ↑. Due to Early effect width of depletion
region ↑ and base width ↓ then recombination in base↑
Small change in α result large change in β
Compare to CB config when CE config o/p char slope is
large
Cut-off region
B-E and C-B both as R.B
IB=0, IC=ICEO (reverse leakage current) which is very small.
25. The region below IB=0 is known as cut-off region
Saturation region
B-E and C-B both as F.B
Region to left of VCE(sat) is called the saturation region.
VCE ↓ very less, then C-B junction as become F.B
Ranges of VCE as 0.1 to 0.3V
26. Transistor parameters
Slope of CB char gives different parameter. Which is
nothing but h-parameter.
i/p impedance
Typical value as 500Ω to 2000Ω
O/p admittance
Typical value as 0.1μΩ to 10μ mho
Forward current gain
Typical value as 20 to 200
Reverse voltage gain
Typical value as 10^-5 to 10^-4
31. I/p Char of CC config as differ from CE and CB config.
The reason as follows
VBC ↑, with VEC=const, then VEB↓ and IB ↓
Which explain slope of CC i/p char.
32. O/p Characteristics
It relates as o/p current (IE) with o/p voltage (VCE) for
varies input current (IB).
Its char is similar to CE configuration.
34. Commonly used transistor connection
CE config only used most 90-95%. The reason as
follows
High current gain
In CE config, IC (o/p)>>IB (i/p) due to large β
So gain is high = 20 to 500
High voltage and power gain
Due to high current gain there will be a high voltage gain
Moderate o/p to i/p impedance relation
In CE config the ratio of o/p impedance to i/p impedance
small (around 50)
This arrangement used to coupling between varies
transistor stages.
35. TWO PORT DEVICES AND HYBRID
MODEL
Behavior of two port model is analyzed using current
and voltage parameter at i/p and o/p port.
Which is namely as Iin, Vin, Io, Vo.
From these
Two parameter as independent
Other two as dependent. Which expressed in terms of
independent parameter
Two port network as shown
36. Here independent variable as i/p current (i1) and o/p
voltage (V2)
i/p voltage (V1) and o/p current i2 can be written as
37. Dimension of h-parameter are as follows
Hybrid parameter as
An alternative subscript notation recommended by IEEE is
commonly used
38. Based on definition of h-parameter the mathematical
model for two-port networks knows as h-parameter
model can be developed as shown.
The above two equation as satisfied by taking KVL in i/p
loop and KCL in o/p loop.
39. h- parameter model of BJT for CE
configuration
In CE configuration
B- i/p terminal
C- o/p terminal
E- common for both i/p and o/p
Dependent variable as--------VB, iC
Independent variable as--------iB, VC
The equation for CE configuration can be written as
40. The h-parameter model for CE configuration is
The subscript “e” indicates that the h-parameters are
for CE-configuration
hie= i/p impedance when C-E terminal is S.C
hre= revere voltage gain when B-E terminal is O.C
hfe= forward current gain when C-E terminal is S.C
hoe= o/p admittance when B-E terminal is O.C
41. h- parameter model of BJT for CB
configuration
In CB configuration
E- i/p terminal
C- o/p terminal
B- common for both i/p and o/p
Dependent variable as--------VE, iC
Independent variable as--------iE, VC
The equation for CB configuration can be written as
42. The h-parameter model for CB configuration is
The subscript “b” indicates that the h-parameters are
for CB-configuration
hib= i/p impedance when C-B terminal is S.C
hrb= revere voltage gain when E- terminal is O.C
hfb= forward current gain when C-B terminal is S.C
hob= o/p admittance when E- terminal is O.C
43. h- parameter model of BJT for CC
configuration
In CC configuration
B- i/p terminal
E- o/p terminal
C- common for both i/p and o/p
Dependent variable as--------VB, iE
Independent variable as--------iB, VE
The equation for CC configuration can be written as
44. The h-parameter model for CC configuration is
The subscript “c” indicates that the h-parameters are
for CC-configuration
hic= i/p impedance when E-C terminal is S.C
hrc= revere voltage gain when B- terminal is O.C
hfc= forward current gain when E-C terminal is S.C
hoc= o/p admittance when B- terminal is O.C
45. ANALYSIS OF A TRANSISTOR
AMPLIFIER CIRCUIT USING h-
PARAMETERS
Basic amplifier circuit as shown fig (1).
For form proper amplifier, then need of connect load
and source circuit with proper biasing
46. This circuit can be replacing with its small signal hybrid
model as shown in fig (2)
For analysis of hybrid model find current gain, i/p
resistance, voltage gain and o/p resistance
48. Current gain (Ais) taking into account the source
resistance Rs:
This model is driven as current source instead of voltage
source and which is given as
49. From this figure (b) using current divider rule get
as follows
50. Input impedance (Zi):
From the figure (2), look at i/p side
It is from figure (1)
55. Power gain (AP):
It is ratio of average power deliver to load RL, to i/p power.
o/p power is given as
56. Conclusion of small signal analysis of a
transistor amplifier as
57.
58. Methods of Transistor Biasing
Following methods are used
Fixed bias (or) Base resistor method
Fixed bias with emitter resistor
Collector-to-Base bias (or) Biasing with feedback
resistor
Collector-Emitter feedback bias
Voltage divider bias (or) Self bias
59. Fixed Bias
Fixed bias circuit as shown
It is also called fixed
current bias or base
resistor biasing circuit.
VCC=VBE=RB=RC=const.
Then IB remains fixed level.
So called fixed bias. For
select proper RB value,
then got IB level.
RB fixed as high (several
100KΩ). For selecting
proper value of RB, then
required value IB can be
made flow
60. Circuit analysis
B-E loop
Write KVL as shown fig, VCC-IBRB_VBE=0, IB=VCC-
VBE/RB
RB value is high, causes more voltage drop across it.
So less drop across B-E jn. So RB set the level of IB.
61. C-E loop
Magnitude of IC=βIB
β =const, then IC is function of IB. Here IC not change w.r.to RC
RC use to find level of VCE.
As per KVL in loop, VCE+ICRC-VCC=0, VCE=VCC-ICRC
So RC set the level of VCE
62. Stability factor (S)
General formula for stability factor as
In a fixed bias IB is independent of IC (i.e) IC=VCC-VBE/RB
So =0, so S=β+1. So stability factor is β+1
times as much as any change in ICO
65. Advantages
It is very simple biasing circuit, as only RB is needed.
Biasing condition can be easily set and calculations are
simple.
Disadvantages
This methods provide poor stabilization. IC ↑, due to temp
not able to control.
Stability factor is very high. So there is strong chances of
thermal runaway.
Due to this demerit, this method of biasing is rarely
used.
66. Fixed bias with Emitter resistor
(Emitter stabilized bias circuit)
Fixed bias emitter resistor
circuit as shown
Also called emitter feedback
bias.
RE introduced to provide better
bias stability.
Current gain β↑ due to temp,
then IC also ↑. It provides more
V.D across RE and ↓ V.D across
RB. Causes IB ↓ and IC ↓.
So if IC ↑ only way to ↑RE.
But practically RE make small
to avoid transistor operate in
67. B-E loop
Apply KVL in loop
The only difference between the equation
Compared in fixed bias as (1+β) RE
71. Collector to Base Bias (DC bias
with voltage feedback)
Also called as Base bias with
collector feedback or collector
feedback bias.
RB connect to C. But it improve
bias stability, V.D across RB
purely depends on VCE.
If IC larger then design value
causes to ↑ V.D across RC. This
result small value of VCE, so that
IB small than design value. Then
IC also ↓.
Although Q-point is not totally
independent of beta, the
sensitivity to changes in beta
79. Advantages
It is simple method and require only RB
This circuit provides stabilization of operating circuit
Disadvantages
This circuit not provide good stabilization because of
stability factor is fairly high, though it is lesser than that
fixed bias. So operating change, due to temp variations
and other effects.
Circuit provide –ve feedback which reduce the gain of
amplifier. During +ve half cycle of signal, IC ↑. Which result
larger drop across RC. This will ↓IB & IC↓
80. Collector –Emitter Feedback Bias
Fig shows C-E f/b circuit
apply both Collector f/b and
Emitter f/b
RB provide Collector f/b
which connect between C &
B
RE provide Emitter f/b which
connect between E &
ground.
Both f/b used to control IC &
IB in opposite direction to
increase stability.
84. Voltage Divider Bias (or) Self
Bias
Also called as self bias (or)
potential divider bias.
Most used method of biasing
and stabilizing the transistor
R1 & R2 connected across Vi
to provide biasing
RE provide stabilization
Voltage divider forms by R1 &
R2. V.D across R2 gives F.B of
B-E junction.
Current flows through RE
causes V.D in which R.B of E-
jn. So transistor remains in
active region
IC↑, due to ICO↑ with temp, IE
↑. So V.D across RE ↑, and
85. Analysis
i/p side of n/w redrawn as shown.
Thevinin equivalent n/w for left of B-terminal can be found
as follows
For finding RTH as shown
86. For finding ETH as shown Thevinin Equivalent circuit as sh
94. Advantages of voltage divider bias over other
types of biasing
In fixed Bias
Stability factor, S=1+β. So β is large, then circuit
provides poor stability
In Collector to Base Bias
RC is very small. S≈1+β. Which is equal to fixed bias.
So this method is not preferable.
In Self Bias
When RB/RE is very small. S≈1 which provides good
stability.
Comparing to other method then voltage
divider method is best method.
95. BJT AS AN AMPLIFIER
A transistor acts as an amplifier by raising the strength of
a weak signal.
The DC bias voltage applied to the emitter base junction
makes it remain in forward biased condition.
This forward bias is maintained regardless of the polarity
of the signal.
The below figure shows how a transistor looks like when
connected as an amplifier. The low resistance in input
circuit lets any small change in input signal to result in an
appreciable change in the output.
The emitter current caused by the input signal
contributes the collector current, which when flows
through the load resistor RL, results in a large voltage
drop across it.
96.
97. SMALL SIGNAL ANALYSIS OF CE
AMPLIFIER
Varies types as
CE amplifier with Fixed Bias
CE amplifier with Unbypassed Emitter Resistor
CE amplifier with Voltage-Divider Bias
CE amplifier with Collector to Base Bias
98. CE amplifier with Fixed Bias
The circuit diagram as shown
The ac equivalent circuit of the amplifier can be drawn
by the steps mentioned as follows
Remove d.c effects of power supply (VCC) by grounding
them
Replace the capacitor (C1 and C2) by S.C
99. Circuit reduces the
equivalent circuit as shown
Substituting the
approximate hybrid
model for the transistor,
the circuit reduces to as
shown
100. Input impedance
Output impedance
It is the impedance
determined with Vi=0. with
Vi=0, Ib=0 and hfeIb=0
indicating an O.C of
current source in
equivalent circuit
Current gain
Voltage gain
101. CE amplifier with Unbypassed Emitter
Resistor
Equivalent circuit as shown AC equivalent amplifier
redrawn as shown
107. CE amplifier with Collector to
Base Bias
The Figure shows the common emitter amplifier with
collector to base bias.
The resistance RF is connected between input and
output.
For the analysis of this circuit it is necessary to split this
resistance for input and output. This can be achieved by
using Miller’s Theorem.
108. Miller’s Theorem:
In general, Miller theorem is used for converting any
circuit having configuration of Figure (a) to another
configuration of Figure (b).
If Z is the impedance connected between two nodes,
node 1 and node 2, it can be replaced by two separate
impedances Z1 and Z2. Where Z1 is connected between
node 1 and ground and Z2 is connected between node 2
and ground.
109. The Vi and V0 are the voltages at the node 1 and
node 2respectively. The values of Z1 and Z2 can
be derived from the ratio of V0 and Vi(V0/Vi),
denoted as k.
The values of impedances Z1 and Z2 are given as,