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FET Biasing 1

FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

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Page 1: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

FET Biasing

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Page 2: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Introduction

For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation.

Nonlinear functions results in curves as obtained for transfer characteristic of a JFET.

Graphical approach will be used to examine the dc analysis for FET because it is most popularly used rather than mathematical approach

The input of BJT and FET controlling variables are the current and the voltage levels respectively

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Page 3: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Introduction

JFETs differ from BJTs:

Nonlinear relationship between input (VGS) and output (ID) JFETs are voltage controlled devices, whereas BJTs are

current controlled

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Page 4: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Introduction

Common FET Biasing Circuits• JFET

– Fixed – Bias – Self-Bias – Voltage-Divider Bias

• Depletion-Type MOSFET– Self-Bias– Voltage-Divider Bias

• Enhancement-Type MOSFET– Feedback Configuration– Voltage-Divider Bias

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Page 5: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

General Relationships For all FETs:

For JFETs and Depletion-Type MOSFETs:

For Enhancement-Type MOSFETs:

5

AIG 0

SD II

2

P

GSDSSD )

V

V(1II

2)( TGSD VVkI

Page 6: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Fixed-Bias Configuration The configuration includes the ac levels Vi and Vo and

the coupling capacitors. The resistor is present to ensure that Vi appears at the

input to the FET amplifier for the AC analysis.

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Page 7: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Fixed-Bias Configuration For the DC analysis,

Capacitors are open circuits and

The zero-volt drop across RG permits replacing RG by a short-circuit

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AIG 0 VRARIV GGGRG 0)0(

Page 8: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Fixed-Bias Configuration

Investigating the input loop

IG=0A, therefore

VRG=IGRG=0V

Applying KVL for the input loop,

-VGG-VGS=0

VGG= -VGS

It is called fixed-bias configuration due to VGG is a fixed

power supply so VGS is fixed

The resulting current,

8

2)1(P

GSDSSD V

VII

Page 9: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Investigating the graphical approach. Using below tables, we can draw the graph

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VGS ID

0 IDSS

0.3VP IDSS/2

0.5 IDSS/4

VP 0mA

Page 10: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

The fixed level of VGS has been superimposed as a

vertical line at

At any point on the vertical line, the level of VG is -VGG---

the level of ID must simply be determined on this vertical

line.

The point where the two curves intersect is the common

solution to the configuration – commonly referrers to as

the quiescent or operating point.

The quiescent level of ID is determine by drawing a

horizontal line from the Q-point to the vertical ID axis.10

GGGS VV

Page 11: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Output loop

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DDDDDS RIVV

VVS 0

SDDS VVV

SDSD VVV 0SV

DSD VV

SGGS VVV

SGSG VVV 0SV

GSG VV

Page 12: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Example

Determine VGSQ, IDQ, VDS, VD, VG, VS

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Page 13: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Exercise

Determine IDQ, VGSQ, VDS, VD, VG and VS

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Page 14: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Self Bias Configuration The self-bias configuration eliminates the need for two

dc supplies. The controlling VGS is now determined by the voltage

across the resistor RS

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Page 15: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

For the indicated input loop:

Mathematical approach:

rearrange and solve.

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SDGS RIV

2

2

1

1

P

SDDSSD

P

GSDSSD

V

RIII

V

VII

Page 16: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Graphical approach Draw the device transfer characteristic Draw the network load line

Use to draw straight line.First point,Second point, any point from ID = 0 to ID = IDSS. Choose

the quiescent point obtained at the intersection of the straight line plot and the device characteristic curve.

The quiescent value for ID and VGS can then be determined and used to find the other quantities of interest.

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SDGS RIV 0,0 GSD VI

2

2

SDSSGS

DSSD

RIV

thenI

I

Page 17: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

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Page 18: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

For output loopApply KVL of output loopUse ID = IS

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RDDDSDSD

SDS

DSDDDDS

VVVVV

RIV

RRIVV

)(

Page 19: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

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Page 20: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

ExampleDetermine VGSQ, IDQ,VDS,VS,VG and VD.

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Page 21: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

ExampleDetermine VGSQ, IDQ, VD,VG,VS and VDS.

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Page 22: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Voltage-Divider Bias The arrangement is the same as BJT but the DC analysis is different In BJT, IB provide link to input and output circuit, in FET VGS does

the same

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Page 23: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Voltage-Divider Bias The source VDD was separated into two equivalent sources to permit

a further separation of the input and output regions of the network.

IG = 0A ,Kirchoff’s current law requires that IR1= IR2 and the series

equivalent circuit appearing to the left of the figure can be used to find the level of VG.

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Page 24: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

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DD2G

RR

VRV

SDGGS

RSGSG

RIVV

VVV

0

Voltage-Divider Bias

VG can be found using the voltage divider rule :

Using Kirchoff’s Law on the input loop:

Rearranging and using ID =IS:

Again the Q point needs to be established by

plotting a line that intersects the transfer curve.24

Page 25: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Procedures for plotting

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1. Plot the line: By plotting two points: VGS = VG, ID =0 and VGS = 0, ID = VG/RS

2. Plot the transfer curve by plotting IDSS, VP and calculated values of ID.

3. Where the line intersects the transfer curve is the Q point for the circuit.

Page 26: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Once the quiescent values of IDQ and VGSQ are determined, the

remaining network analysis can be found.

Output loop:

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2121 RR

VII DDRR

)( SDDDDDDS RIRIVV

DDDDD RIVV

SDS RIV

Page 27: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

Effect of increasing values of RS

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Page 28: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

ExampleDetermine IDQ, VGSQ, VD, VS, VDS and VDG.

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Page 29: FET Biasing 1. Introduction For the JFET, the relationship between input and output quantities is nonlinear due to the squared term in Shockley’s equation

ExampleDetermine IDQ, VGSQ, VDS, VD and VS

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