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JFET Junction Field Effect Transistor
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Jfet

Apr 13, 2017

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Mohammad Akram
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Page 1: Jfet

JFET

Junction Field Effect Transistor

Page 2: Jfet

Introduction (FET) Field-effect transistor (FET) are important

devices such as BJTs Also used as amplifier and logic switches What is the difference between JFET and

BJT?

Page 3: Jfet

BJT is Current-controlled

Page 4: Jfet

FET is Voltage-controlled

Page 5: Jfet

Types of Field Effect Transistors (The Classification)

JFET

MOSFET (IGFET)

n-Channel JFETp-Channel JFET

n-Channel EMOSFET

p-Channel EMOSFET

Enhancement MOSFET

Depletion MOSFET

n-Channel DMOSFET

p-Channel DMOSFET

FET

Page 6: Jfet

High input impedance (M) (Linear AC amplifier system)

Temperature stable than BJT Smaller than BJT Can be fabricated with fewer processing BJT is bipolar – conduction both hole and electron FET is unipolar – uses only one type of current

carrier Less noise compare to BJT Usually use as an Amplifier and logic switch

Introduction.. (Advantages of FET over BJT)

Page 7: Jfet

Disadvantages of FET Easy to damage compare to BJT

Page 8: Jfet

There are 2 types of JFET n-channel JFET p-channel JFET

Three Terminal Drain – D Gate -G Source – S

Junction field-effect transistor..

Page 9: Jfet

Gate

Drain

Source

SYMBOLS

n-channel JFET

Gate

Drain

Source

p-channel JFET

Page 10: Jfet

N channel JFET: Major structure is n-type material (channel)

between embedded p-type material to form 2 p-n junction.

In the normal operation of an n-channel device, the Drain (D) is positive with respect to the Source (S). Current flows into the Drain (D), through the channel, and out of the Source (S)

Because the resistance of the channel depends on the gate-to-source voltage (VGS), the drain current (ID) is controlled by that voltage

N-channel JFET

Page 11: Jfet

N-channel JFET..

Page 12: Jfet

P channel JFET: Major structure is p-type material

(channel) between embedded n-type material to form 2 p-n junction.

Current flow : from Source (S) to Drain (D)

Holes injected to Source (S) through p-type channel and flowed to Drain (D)

P-channel JFET

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P-channel JFET..

Page 14: Jfet

Water analogy for the JFET control mechanism

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Page 16: Jfet

JFET Characteristic for VGS = 0 V and 0<VDS<|Vp|

To start, suppose VGS=0 Then, when VDS is increased, ID increases. Therefore,

ID is proportional to VDS for small values of VDS For larger value of VDS, as VDS increases, the

depletion layer become wider, causing the resistance of channel increases.

After the pinch-off voltage (Vp) is reached, the ID becomes nearly constant (called as ID maximum, IDSS-Drain to Source current with Gate Shorted)

Page 17: Jfet

JFET for VGS = 0 V and 0<VDS<|Vp|

Channel becomes narrower as VDS is increased

Page 18: Jfet

Pinch-off (VGS = 0 V, VDS = VP).

Page 19: Jfet

ID versus VDS

JFET Characteristic Curve

for VGS = 0 V and 0<VDS<|Vp|

Page 20: Jfet

(Application of a negative voltage to the gate of a JFET) JFET for

Page 21: Jfet

JFET Characteristic Curve.. For negative values of VGS, the gate-to-channel junction

is reverse biased even with VDS=0 Thus, the initial channel resistance of channel is

higher. The resistance value is under the control of VGS

If VGS = pinch-off voltage(VP) The device is in cutoff (VGS=VGS(off) = VP) The region where ID constant – The saturation/pinch-off

region The region where ID depends on VDS is called the

linear/ohmic region

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Page 23: Jfet

p-Channel JFET

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p-Channel JFET characteristics with IDSS = 6 mA and VP = +6 V.

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Characteristics for n-channel JFET

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P

+

++

Characteristics for p-channel JFET

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Page 28: Jfet

Transfer Characteristics

The input-output transfer characteristic of the JFET is not as straight forward as it is for the BJT. In BJT:

IC= IB

which is defined as the relationship between IB (input current) and IC (output current).

Page 29: Jfet

Transfer Characteristics..In JFET, the relationship between VGS (input voltage) and ID (output current) is used to define the transfer characteristics. It is called as Shockley’s Equation:

The relationship is more complicated (and not linear)As a result, FET’s are often referred to a square law devices

2GS

D DSSP

V I = I 1 - V

VP=VGS (OFF)

Page 30: Jfet

Defined by Shockley’s equation:

Relationship between ID and VGS. Obtaining transfer characteristic curve axis

point from Shockley: When VGS = 0 V, ID = IDSS

When VGS = VGS(off) or Vp, ID = 0 mA

)(

2

)(

1 offGSPoffGS

GSDSSD VV

VVII

Transfer Characteristics…

Page 31: Jfet

Transfer Characteristics

JFET Transfer Characteristic Curve JFET Characteristic Curve

Page 32: Jfet

Exercise 1

DGS P

DSS

I V = V 1 - I

2GS

D DSSP

V I = I 1 - V

VGS ID0 IDSS

0.3Vp IDSS/20.5Vp IDSS/4

Vp 0 mA

Sketch the transfer defined byIDSS = 12 mA dan VGS(off) = - 6

Page 33: Jfet

Exercise 1

DGS P

DSS

I V = V 1 - I

Sketch the transfer defined by IDSS = 12 mA dan VGS(off) = Vp= - 6 IDSS

IDSS/2IDSS/4

2GS

D DSSP

V I = I 1 - V

VGS =0.3VP

VGS =0.5VP

Page 34: Jfet

Answer 1

Page 35: Jfet

Exercise 2

DGS P

DSS

I V = V 1 - I

2GS

D DSSP

V I = I 1 - V

VGS ID0 IDSS

0.3Vp IDSS/20.5Vp IDSS/4

Vp 0 mA

Sketch the transfer defined byIDSS = 4 mA dan VGS(off) = 3 V

Page 36: Jfet

Exercise 2

DGS P

DSS

I V = V 1 - I

Sketch the transfer defined by IDSS = 4 mA dan VGS(off) = 3V

2GS

D DSSP

V I = I 1 - V

VGS =0.5VP

VGS =0.3VP

VP

IDSS

IDSS/2IDSS/4

Page 37: Jfet

Answer 2Answer 2