7
f = XC 0 Ri Ro Av Ri = vi ii RL=Ro Av = vo vi RL=n p gm = g fs = y fs = ∂ID ∂VGS Q r ds = 1 gos = 1 yos = ∂VDS ∂ID Q gm r ds 6= μ = gmr ds gm 1 5 r ds 20 Ω 100 Ω μ 20 500 g m gm gm = ∂ID ∂VGS Q = ΔID ΔVGS Q gm I gm ID = IDSS 1 - VGS VP 2 gm = ∂ID ∂VGS Q = 2IDSS |VP | 1 - VGS VP Q = 2IDSS |VP | 1 - VGSQ VP = 2IDSS |VP | s IDQ IDSS ...IDQ = IDSS 1 - VGSQ VP 2 = gm0 s IDQ IDSS ...gm0 = 2IDSS |VP | I gm ID = k ( VGS - V GS(Th) ) 2 gm = ∂ID ∂VGS Q =2k ( VGS - V GS(Th) ) Q =2k ( VGSQ - V GS(Th) ) =2 k p IDQ ...IDQ = k ( VGS - V GS(Th) ) 2

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Page 1: FET Small-Signal Model - Hacettepe Universityusezen/ele230/FET-6sp.pdf · FET Small-Signal AnalysisFET Small-Signal Model FET Small-Signal Model Small-signal equivalent model for

Contents

FET Small-Signal AnalysisFET SSAC Analysis Steps

FET Small-Signal Model

Common-Source Fixed-Bias CongurationInput Resistance

Voltage Gain

Output Resistance

Common-Source Self-Bias CongurationInput Resistance

Voltage Gain

Output Resistance

Common-Source Voltage-Divider Bias CongurationInput Resistance

Voltage Gain

Output Resistance

Common-Source Unbypassed Self-Bias CongurationInput Resistance

Voltage Gain

Output Resistance

Source-Follower CongurationInput Resistance

Voltage Gain

Output Resistance

Common-Source Drain Feedback CongurationInput Resistance

Voltage Gain

Output Resistance

Common-Gate CongurationInput Resistance

Voltage Gain

Output Resistance

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 1 / 42

FET Small-Signal Analysis

FET SSAC Analysis Steps

1. Draw the SSAC equivalent circuit

a) Draw the AC equivalent circuit (signal frequency is innity, i.e., f =∞)

i. Capacitors are short circuit, i.e., XC → 0.ii. Kill the DC power sources (i.e., AC value of DC sources is zero).

b) Replace FET with its small-signal equivalent model.

2. Calculate the three amplier parameters: Ri, Ro and Av

a) Calculate no-load input resistance, Ri = viii

∣∣∣RL=∞

.

b) Calculate output resistance, Ro.

c) Calculate no-load voltage gain, Av = vovi

∣∣∣RL=∞

.

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 2 / 42

FET Small-Signal Analysis FET Small-Signal Model

FET Small-Signal ModelSmall-signal equivalent model for a FET transistor is provided below. This model and its analysisis the same for all FET types, i.e., JFET, DMOSFET, EMOSFET, n-channel and p-channel.

Here,

gm = gfs = yfs =∂ID

∂VGS

∣∣∣∣Q-point

is the forward transfer conductance,

rds =1

gos=

1

yos=

∂VDS

∂ID

∣∣∣∣Q-point

is the output resistance.

Forward transfer conductance gm is mostly called as the transconductance parameter.

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 3 / 42

FET Small-Signal Analysis FET Small-Signal Model

When rds 6=∞, we can also use the voltage-controlled voltage source model (viaNorton-to-Thévenin transformation, a.k.a source transformation) as shown below. We mostlyuse this model for the common-gate and unbypassed self-bias congurations.

Here µ = gmrds is the forward transfer-voltage gain.

Typical values of gm run from 1mS to 5mS,

Typical values of rds run from 20 kΩ to 100 kΩ,

Consequently, typical values of µ run from 20 to 500.

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 4 / 42

FET Small-Signal Analysis FET Small-Signal Model

Transconductance Parameter (gm)Transconductance parameter gm is given by

gm =∂ID

∂VGS

∣∣∣∣Q-point

∼=∆ID

∆VGS

∣∣∣∣Q-point

In other words, gm is the slope of the characteristics at the point of operation as shown below.

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 5 / 42

FET Small-Signal Analysis FET Small-Signal Model

I Let us derive gm for the JFET equation, ID = IDSS

(1− VGS

VP

)2gm =

∂ID

∂VGS

∣∣∣∣Q-point

=2IDSS

|VP |

(1−

VGS

VP

)∣∣∣∣Q-point

=2IDSS

|VP |

(1−

VGSQ

VP

)

=2IDSS

|VP |

√IDQ

IDSS. . . IDQ = IDSS

(1−

VGSQ

VP

)2

= gm0

√IDQ

IDSS. . . gm0 =

2IDSS

|VP |

I Let us derive gm for the MOSFET equation, ID = k(VGS − VGS(Th)

)2gm =

∂ID

∂VGS

∣∣∣∣Q-point

= 2k(VGS − VGS(Th)

)∣∣Q-point

= 2k(VGSQ − VGS(Th)

)= 2√k√IDQ . . . IDQ = k

(VGS − VGS(Th)

)2

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 6 / 42

Page 2: FET Small-Signal Model - Hacettepe Universityusezen/ele230/FET-6sp.pdf · FET Small-Signal AnalysisFET Small-Signal Model FET Small-Signal Model Small-signal equivalent model for

FET Small-Signal Analysis FET Small-Signal Model

Phase RelationshipThe phase relationship between input and output depends on the amplier conguration circuitas listed below.

Common-Source: 180 degrees

Common-Gate: 0 degrees

Common-Drain: 0 degrees (Source-Follower)

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 7 / 42

FET Small-Signal Analysis Common-Source Fixed-Bias Conguration

Common-Source Fixed-Bias CongurationCommon-source xed-bias conguration is given below

Corresponding SSAC equivalent circuit is shown below

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 8 / 42

FET Small-Signal Analysis Common-Source Fixed-Bias Conguration

Input Resistance

Input resistance Ri is given as

Ri =vi

ii

∣∣∣∣RL=∞

= RG

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 9 / 42

FET Small-Signal Analysis Common-Source Fixed-Bias Conguration

Voltage Gain

No-load voltage gain Av is given by

Av =vo

vi

∣∣∣∣RL=∞

=

(vo

gmvgs

)(gmvgs

vgs

)(vgs

vi

)= (−RD||rds) (gm) (1)

= −gm (RD||rds)

If rds ≥ 10RD, voltage gain Av reduces to

Av = −gmRD

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 10 / 42

FET Small-Signal Analysis Common-Source Fixed-Bias Conguration

For the circuit above, we can obtain the current gain Ai as follows

Ai =io

ii=vo/RD

vi/Ri=

Ri

RD

vo

vi

=Ri

RDAv

If rds ≥ 10RD, current gain Ai reduces to

Ai = −gmRG

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 11 / 42

FET Small-Signal Analysis Common-Source Fixed-Bias Conguration

Output Resistance

Output resistance, i.e., Thévenin equivalent resistance, Ro is calculated using the testvoltage circuit above. Note that in the circuit vgs = 0, so gmvgs = 0 as well.

Ro =vtest

itest

∣∣∣∣vs=0,RL=vtest

= RD||rds

If rds ≥ 10RD, then Ro simplies to Ro = RD.

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 12 / 42

Page 3: FET Small-Signal Model - Hacettepe Universityusezen/ele230/FET-6sp.pdf · FET Small-Signal AnalysisFET Small-Signal Model FET Small-Signal Model Small-signal equivalent model for

FET Small-Signal Analysis Common-Source Self-Bias Conguration

CS Self-Bias CongurationCommon-source self-bias conguration is given below

Corresponding SSAC equivalent circuit is shown below

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 13 / 42

FET Small-Signal Analysis Common-Source Self-Bias Conguration

Input Resistance

Input resistance Ri is given as

Ri =vi

ii

∣∣∣∣RL=∞

= RG

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 14 / 42

FET Small-Signal Analysis Common-Source Self-Bias Conguration

Voltage Gain

No-load voltage gain Av is given by

Av =vo

vi

∣∣∣∣RL=∞

=

(vo

gmvgs

)(gmvgs

vgs

)(vgs

vi

)= (−RD||rds) (gm) (1)

= −gm (RD||rds)

If rds ≥ 10RD, no-load voltage gain Av reduces to

Av = −gmRD

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 15 / 42

FET Small-Signal Analysis Common-Source Self-Bias Conguration

For the circuit above, we can obtain the current gain Ai as follows

Ai =io

ii=vo/RD

vi/Ri=

Ri

RD

vo

vi

=Ri

RDAv

If rds ≥ 10RD, current gain Ai reduces to

Ai = −gmRG

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 16 / 42

FET Small-Signal Analysis Common-Source Self-Bias Conguration

Output Resistance

Output resistance, i.e., Thévenin equivalent resistance, Ro is calculated using the testvoltage circuit above. Note that in the circuit vgs = 0, so gmvgs = 0 as well.

Ro =vtest

itest

∣∣∣∣vs=0,RL=vtest

= RD||rds

If rds ≥ 10RD, then Ro simplies to Ro = RD.

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 17 / 42

FET Small-Signal Analysis Common-Source Voltage-Divider Bias Conguration

CS Voltage-Divider Bias CongurationCommon-source voltage-divider bias conguration is given below

Corresponding SSAC equivalent circuit is shown below

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 18 / 42

Page 4: FET Small-Signal Model - Hacettepe Universityusezen/ele230/FET-6sp.pdf · FET Small-Signal AnalysisFET Small-Signal Model FET Small-Signal Model Small-signal equivalent model for

FET Small-Signal Analysis Common-Source Voltage-Divider Bias Conguration

Input Resistance

Input resistance Ri is given as

Ri =vi

ii

∣∣∣∣RL=∞

= R1||R2

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 19 / 42

FET Small-Signal Analysis Common-Source Voltage-Divider Bias Conguration

Voltage Gain

No-load voltage gain Av is given by

Av =vo

vi

∣∣∣∣RL=∞

=

(vo

gmvgs

)(gmvgs

vgs

)(vgs

vi

)= (−RD||rds) (gm) (1)

= −gm (RD||rds)

If rds ≥ 10RD, no-load voltage gain Av reduces to

Av = −gmRD

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 20 / 42

FET Small-Signal Analysis Common-Source Voltage-Divider Bias Conguration

For the circuit above, we can obtain the current gain Ai as follows

Ai =io

ii=vo/RD

vi/Ri=

Ri

RD

vo

vi

=Ri

RDAv

If rds ≥ 10RD, current gain Ai reduces to

Ai = −gm (R1||R2)

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 21 / 42

FET Small-Signal Analysis Common-Source Voltage-Divider Bias Conguration

Output Resistance

Output resistance, i.e., Thévenin equivalent resistance, Ro is calculated using the testvoltage circuit above. Note that in the circuit vgs = 0, so gmvgs = 0 as well.

Ro =vtest

itest

∣∣∣∣vs=0,RL=vtest

= RD||rds

If rds ≥ 10RD, then Ro simplies to Ro = RD.

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 22 / 42

FET Small-Signal Analysis Common-Source Unbypassed Self-Bias Conguration

CS Unbypassed Self-Bias Conguration

Common-source unbypassed self-bias conguration and its SSAC equivalent circuit aregiven on the left and right gures below, respectively.

When RS is not bypassed, we normally use the voltage-controlled voltage source model inthe small-signal equivalent circuit as shown above.

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 23 / 42

FET Small-Signal Analysis Common-Source Unbypassed Self-Bias Conguration

Input Resistance

Input resistance Ri is given as

Ri =vi

ii

∣∣∣∣RL=∞

= RG

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 24 / 42

Page 5: FET Small-Signal Model - Hacettepe Universityusezen/ele230/FET-6sp.pdf · FET Small-Signal AnalysisFET Small-Signal Model FET Small-Signal Model Small-signal equivalent model for

FET Small-Signal Analysis Common-Source Unbypassed Self-Bias Conguration

Voltage Gain

No-load voltage gain Av is given by

Av =vo

vi

∣∣∣∣RL=∞

=

(vo

id

)(id

vgs

)(vgs

vi

)

= (−RD)

RS + RD + rds

)(vgs

vgs + idRS

). . . id =

µvgs

RS + RD + rds

= (−RD)

RS + RD + rds

) 1

1 +µRS

RS+RD+rds

= −

µRD

(µ+ 1)RS + RD + rds. . . µ = gmrds

= −gmRD

1 + gmRS +RS+RDrds

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 25 / 42

FET Small-Signal Analysis Common-Source Unbypassed Self-Bias Conguration

If rds ≥ 10 (RD +RS), no-load voltage gain Av reduces to

Av = −gmRD

1 + gmRS

If rds ≥ 10 (RD +RS) and gmRS 1, no-load voltage gain Av reduces to

Av ≈ −RD

RS

For the circuit above, we can obtain the current gain Ai as follows

Ai =io

ii=vo/RD

vi/Ri=

Ri

RD

vo

vi

=Ri

RDAv

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 26 / 42

FET Small-Signal Analysis Common-Source Unbypassed Self-Bias Conguration

Output Resistance

Output resistance, i.e., Thévenin equivalent resistance, Ro is calculated using the testvoltage circuit above.

Ro =vtest

itest

∣∣∣∣vs=0,RL=vtest

=vtest

vtestRD

+ id. . . itest = iRD + id

=vtest

vtestRD

− vgsRS

. . . vs = −vgs, id =−vgsRS

=vtest

vtestRD

+ vtest(µ+1)RS+rds

. . . vgs = −vtest

(µ+ 1) + rds/RS

= RD|| [(µ+ 1)RS + rds] . . . µ = gmrds

= RD|| [(gmRS + 1) rds +RS ]

∼= RD

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 27 / 42

FET Small-Signal Analysis Source-Follower Conguration

Source-Follower Conguration

Source-follower (common-drain) conguration is given below

Corresponding SSAC equivalent circuit is shown below

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 28 / 42

FET Small-Signal Analysis Source-Follower Conguration

Input Resistance

Input resistance Ri is given as

Ri =vi

ii

∣∣∣∣RL=∞

= RG

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 29 / 42

FET Small-Signal Analysis Source-Follower Conguration

Voltage Gain

No-load voltage gain Av is given by

Av =vo

vi

∣∣∣∣RL=∞

=

(vo

vgs

)(vgs

vi

)= [gm (RS ||rds)]

(1

1 + gm (RS ||rds)

). . . vi = vgs + vo

=gm (RS ||rds)

1 + gm (RS ||rds)∼= 1

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 30 / 42

Page 6: FET Small-Signal Model - Hacettepe Universityusezen/ele230/FET-6sp.pdf · FET Small-Signal AnalysisFET Small-Signal Model FET Small-Signal Model Small-signal equivalent model for

FET Small-Signal Analysis Source-Follower Conguration

For the circuit above, we can obtain the current-gain Ai as follows

Ai =io

ii=vo/RS

vi/Ri=

Ri

RS

vo

vi

=Ri

RSAv

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 31 / 42

FET Small-Signal Analysis Source-Follower Conguration

Output Resistance

Output resistance, i.e., Thévenin equivalent resistance, Ro is calculated using the test voltage

circuit above.

Ro =vtest

itest

∣∣∣∣vs=0,RL=vtest

=vtest

vtestRS ||rds

− gmvgs. . . itest = iRS ||rds − gmvgs

=vtest

vtestRS ||rds

+ gmvtest. . . vtest = −vgs

=vtest

vtestRS ||rds

+vtest1/gm

= RS ||rds||1

gmIf (RS ||rds) ≥ 10/gm, output resistance Ro reduces to

Ro ∼=1

gm

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 32 / 42

FET Small-Signal Analysis Common-Source Drain Feedback Conguration

CS Drain Feedback CongurationCommon-source drain feedback bias conguration is given below

Corresponding SSAC equivalent circuit is shown below

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 33 / 42

FET Small-Signal Analysis Common-Source Drain Feedback Conguration

Input Resistance

Input resistance Ri is given as

Ri =vi

ii

∣∣∣∣RL=∞

=vgs

gmvgs + vo/ (RD||rds). . . vi = vgs

=RF +RD||rds

1 + gm (RD||rds). . . vo =

(1− gmRF ) (RD||rds) vgsRF +RD||rds

∼=RF

1 + gm (RD||rds). . . RF RD||rds

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 34 / 42

FET Small-Signal Analysis Common-Source Drain Feedback Conguration

Voltage Gain

No-load voltage gain Av is given by

Av =vo

vi

∣∣∣∣RL=∞

=(1− gmRF ) (RD||rds)

RF +RD||rds. . . vi = vgs

∼= −gm (RD||rds||RF ) . . . gmRF 1

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 35 / 42

FET Small-Signal Analysis Common-Source Drain Feedback Conguration

For the circuit above, we can obtain the current-gain Ai as follows

Ai =io

ii=vo/RD

vi/Ri=

Ri

RD

vo

vi

=Ri

RDAv

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 36 / 42

Page 7: FET Small-Signal Model - Hacettepe Universityusezen/ele230/FET-6sp.pdf · FET Small-Signal AnalysisFET Small-Signal Model FET Small-Signal Model Small-signal equivalent model for

FET Small-Signal Analysis Common-Source Drain Feedback Conguration

Output Resistance

Output resistance, i.e., Thévenin equivalent resistance, Ro is calculated using the testvoltage circuit above. Note that in the circuit vgs = 0, so gmvgs = 0 as well.

Ro =vtest

itest

∣∣∣∣vs=0,RL=vtest

= RD||rds||RF

If a voltage source with source resistance Rs is connected to the input, replace RF with[(RF +Rs) / (1 + gmRs)] in Ro calculations.

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 37 / 42

FET Small-Signal Analysis Common-Gate Conguration

Common-Gate Conguration

Common-gate conguration is given below

Corresponding SSAC equivalent circuit is shown below

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 38 / 42

FET Small-Signal Analysis Common-Gate Conguration

Input Resistance

Input resistance Ri is given as

Ri =vi

ii

∣∣∣∣RL=∞

=vi

vi/RS − id. . . vi = −vgs

=vi

vi/RS + vi/(RD+rdsµ+1

) . . . id =(µ+ 1) vgs

RD + rds

= RS ||RD + rds

1 + gmrds. . . µ = gmrds

∼= RS ||1

gm. . . rds ≥ 10RD and gmrds 1

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 39 / 42

FET Small-Signal Analysis Common-Gate Conguration

Voltage Gain

No-load voltage gain Av is given by

Av =vo

vi

∣∣∣∣RL=∞

=−idRD−vgs

. . . vi = −vgs

=(µ+ 1)RD

RD + rds. . . id =

(µ+ 1) vgs

RD + rds

=(gmrds + 1)RD

RD + rds. . . µ = gmrds

∼= gmRD . . . rds ≥ 10RD and gmrds 1

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 40 / 42

FET Small-Signal Analysis Common-Gate Conguration

For the circuit above, we can obtain the current-gain Ai as follows

Ai =io

ii=vo/RD

vi/Ri=

Ri

RD

vo

vi

=Ri

RDAv

If rds ≥ 10RD and gmrds 1, current-gain Ai reduces to

Ai = gm

(RS ||

1

gm

)≈ 1

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 41 / 42

FET Small-Signal Analysis Common-Gate Conguration

Output Resistance

Output resistance, i.e., Thévenin equivalent resistance, Ro is calculated using the testvoltage circuit above. Note that in the circuit vgs = 0, so gmvgs = 0 as well.

Ro =vtest

itest

∣∣∣∣vs=0,RL=vtest

= RD||rds

If rds ≥ 10RD, then Ro simplies to Ro = RD.

If a voltage source with source resistance Rs is connected to the input, replace rds with([1 + gm (Rs||RG)] rds +Rs||RG) in Ro calculations. We can say that Ro ≈ RD inmost cases.

Dr. U. Sezen & Dr. D. Gökcen (Hacettepe Uni.) ELE230 Electronics I 24-Apr-2018 42 / 42