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IDEAL INSTITUTE OF ENGINEERING

NAME - KALYAN MONDAL


ROLL - 27901621046
DEPARMENT - ELECTRICAL
YEAR- - 3RD YEAR(5TH SEM)
SUBJECT - POWER ELECTRONIC
TOPIC - WORKING PRINCIPAL OF
POWER TRANSISTOR
INTRODUCTION
What is transistor?
A three-terminal device whose output current, voltage
and/or power are controlled by its input.

Commonly used in audio application as an amplifier, in


switching application as a switch and in power supply
voltage and current regulator circuit.

2 basic transistor types: BJT and FET


These two transistor differ in their operating
characteristic and their internal construction.
Transistor Currents
 The directions of the currents in npn transistor and
pnp transistor are shown in the figure.
 The emitter current (IE) is the sum of the collector
current (IC) and the base current (IB)
 IB << IE or IC
 The capital letter – dc value
 Transistor is a current-controlled device - the value of
collector and emitter currents are determined by the
value of base current.
 An increase or decrease in value of IB causes similar
change in values of IC and IE.
Transistor Voltages
 VCC – collector supply voltage. This is a power supply
voltage applied directly to collector of transistor.
 VBB – base supply voltage. this is dc voltage used to bias
base of transistor.
 VEE – emitter supply voltage. dc biasing voltage and in
many cases, VEE is simply a ground connection.
BJT OPERATION
To operate the transistor properly, the two pn
junction must be correctly biased with external dc
voltages.
The figure shown the proper bias arrangement for
both npn and pnp transistor for active operation as
an amplifier.
Transistor is made of 3 separate semiconductor
materials that joined together to form two pn
junction.
Point at which emitter and base are joined forms a
single pn junction  base-emitter junction
Collector-base junction  point where base and
collector meet.
Cutoff region
Both transistor
junctions are reverse
biased.
With large depletion
region between C-B and
E-B, very small amount
of reverse current, ICEO
passes from emitter to
collector and can be
neglected.
So, VCE = VCC
Saturation region

 Both transistor junctions are


forward-biased.
 IC reaches its maximum
value as determined by VCC
and total resistance in C-E
circuit.
 IC is independently from
relationship of β and IB.
 VBE is approximately 0.7V
and VCE < VBE. VCC
IC 
RC  RE
Active region
BE junction is forward
biased and the BC
junction is reverse biased.
All terminal currents have
some measurable value.
The magnitude of IC
depends on the values of
β and IB.
VCE is approximately near
to 0.7V and VCE falls in
ranges VBE<VCE<VCC.
Summary
A transistor can be operated as an electronics
switch.
When the transistor is off it is in cutoff condition
(no current).
 When the transistor is on, it is in saturation
condition (maximum current).
 Beta can vary with temperature and also varies
from transistor to transistor.

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