This document provides an overview of the Junction Field Effect Transistor (JFET). It discusses the construction of JFETs including the source, drain and gate terminals. It describes the theory of operation explaining how applying voltages to the gate can control the channel and current flow. The key sections outline the characteristic I-V curve, pinch-off voltage, saturation level and cut-off voltage. Advantages of JFETs are also summarized such as high input impedance. Common applications are listed including use as amplifiers and constant current sources.
Advised by :
Engr.Md Asif Mahmood Chowdhury
Prepared by :
Sayed Mohammad Jahed Hossain ET - 101003
Ishtiaque Ahmed ET - 101014
Md. Ashraf Uddin Chowdhury ET - 101015
Mokammel Hossain ET - 101017
2.
Field EffectTransistor (FET)
Junction Field Effect Transistor (JFET)
Construction of JFET
Theory of Operation
I-V Characteristic Curve
Pinch off Voltage (VP)
Saturation Level
Break Down Region
Ohmic Region
Cut off Voltage
Advantages
Disadvantages
Application of JFET
OUTLINE
3.
INTRODUCTION
The ordinary orbipolar transistor has two main disadvantage.
• It has a low input impedance
• It has considerable noise level
To overcome this problem Field effect transistor (FET) is introduced
because of its:
• High input impedance
• Low noise level than ordinary transistor
And Junction Field Effect Transistor (JFET) is a type of FET.
4.
FET
FET isa voltage controled device.
It consists of three terminal .
• Gate
• Source
• Drain
It is classified as four types.
JFET
MESFET MISFET
MOSFET
Field Effect Transistor (FET)
5.
Junction FieldEffect Transistor is a three terminal semiconductor device in which
current conducted by one type of carrier i.e. by electron or hole.
Junction Field Effect Transistor (JFET)
6.
Source: Theterminal through which the
majority carriers enter into the channel, is
called the source terminal S .
Drain: The terminal, through which the
majority carriers leave from the channel, is
called the drain terminal D .
Gate: There are two internally connected
heavily doped impurity regions to create two
P-N junctions. These impurity regions are
called the gate terminal G.
Channel: The region between the source
and drain, sandwiched between the two gates
is called the channel .
Construction of JFET
JFET isa voltage controlled device i.e. input voltage (VGS) control the
output current (ID).
In JFETs, the width of a junction is used to control the effective cross-
sectional area of the channel through which current conducts.
It is always operated with Gate-Source p-n junction in reverse bias.
Because of reverse bias it has high input impedance.
In JFET the gate current is zero i.e. IG=0.
Features of JFET
10.
(i) When gate-sourcevoltage(VGS) is applied and drain-source voltage is zero i.e. VDS= 0V
When VGS = 0v , two depletion layers & channel are formed normally.
When VGS increase negatively i.e. 0V > VGS > VGS(off) , depletion layers are also increased and
channel will be decrease.
When VGS=VGS(off), depletion layer will touch each other and channel will totally removed. So no
current can flow through the channel.
Theory of Operation
Depletion layer
11.
(ii) When drain-sourcevoltage (VDS) is applied at constant gate-source voltage (VGS) :
Now reverse bias at the drain end is larger than
source end and so the depletion layer is wider at
the drain end than source end.
When VDS increases i.e. 0v < VDS < VP , depletion layer at
drain end is gradually increased and drain current also
increased.
When VDS = VP the channel is effectively closed at drain
end and it does not allow further increase of drain
current. So the drain current will become constant.
Theory of Operation
12.
It is thecurve between drain current (ID)and drain-source voltage (VDS)for different
gate-source voltage (VGS). It can be characterized as:
For VGS=0v the drain current is maximum. It’s denoted as IDSS and called shorted
gate drain current.
Then if VGS increases Drain current ID decreases (ID < IDSS) even though VDS is
increased.
When VGS reaches a certain value, the drain current will be decreased to zero.
For different VGS, the ID will become constant after pinch off voltage (VP) though
VDS is increased.
I-V Characteristic Curve
13.
Fig: Transfer CharacteristicCurve
Transfer Characteristic Curve
This curve shows the value of ID for a given value of VGS .
14.
It isthe minimum drain source voltage at which the drain current essentially
become constant.
Pinch off Voltage (VP)
Pinch off Voltage
15.
After pinchoff voltage the drain current become constant, this constant level is
known as saturation level .
Saturation Level
Saturation Level
16.
The regionbehind the pinch off voltage where the drain current increase rapidly is
known as Ohmic Region.
Ohmic Region
17.
Break Down Region
It is the region, when the drain-source voltage (VDS) is high enough to cause the
JFET’s resistive channel to breakdown and pass uncontrolled maximum current .
18.
The gate-sourcevoltage, when the drain current become zero is called cut-
off voltage. Which is usually denoted as VGS(off).
Cut off Voltage
Here ID become Zero
19.
It issimpler to fabricate, smaller in size.
It has longer life and higher efficiency.
It has high input impedance.
It has negative temperature coefficient of resistance .
It has high power gain.
Advantages