8. Biasing Transistor Amplifiersaries.ucsd.edu/NAJMABADI/CLASS/ECE65/13-W/Slides/ECE65_W13-8-Bias.pdfIssues in developing a transistor amplifier: F. Najmabadi, ECE65, Winter 2013,

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8. Biasing Transistor Amplifiers

Lecture notes: Sec. 5

Sedra & Smith (6th Ed): Sec. 5.4, 5.6 & 6.3-6.4 Sedra & Smith (5th Ed): Sec. 4.4, 4.6 & 5.3-5.4

ECE 65, Winter2013, F. Najmabadi

Issues in developing a transistor amplifier:

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (2/29)

1. Find the iv characteristics of the elements for the signal (which can be different than their characteristics equation for bias). o This will lead to different circuit configurations for bias versus signal

2. Compute circuit response to the signal o Focus on fundamental transistor amplifier configurations

3. How to establish a Bias point (bias is the state of the system when there is no signal). o Stable and robust bias point should be resilient to variations in

µnCox (W/L),Vt (or β for BJT) due to temperature and/or manufacturing variability.

o Bias point details impact small signal response (e.g., gain of the amplifier).

BJT biasing with Base Voltage (Fixed Bias)

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (3/29)

B

DBBB

BEBBBB

RVVI

VRIV

0

:KVLBE−

=

+=−

* Typically VBB = VCC in order to reduce the need for additional reference voltages.

)(

:KVLCE

0DBBB

CCCCE

CECCCC

VVRRVV

VRIV

−−=

+=−β

B

DBBBC R

VVII 0 −== ββ

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (4/29)

Exercise 1: Find RC and RB such that BJT would be in active with VCE = 5V and IC = 25 mA. (VCC = 15 V, Si BJT with β = 100 and VA = ∞).

Ω=+×=+=− −

400 5102551 :KVLCE 3

C

CCECC

RRVRI

V 7.05 and 0 since Activein is BJT 0 =≥=> DCEC VVI

mA 25.0 / == βCB II

k 2.57 7.01025.051 :KVLBE 3

=+×=+=− −

B

BBEBB

RRVRI

Exercise 2: Consider the circuit designed in Exercise 1 (RC = 400 , RB = 57.2 k, VCC = 15 V ). Find the operating point of BJT if β = 200.

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (5/29)

mA 25.0 7.0102.5751 :KVLBE 3

=+×=+=−

B

BBEBB

IIVRI

V 7.0 and 0 V, 7.0: Activein is BJT Assume

≥>= CECBE VIV

V 5 400105051 :KVLCE 3

−=+××=+=− −

CE

CECECC

VVVRI

mA 50 == BC II β

BJT in saturation! Note, compared to Exercise 1:

IB is the same.

IC has increased.

VCE had decreased.

Why biasing with base voltage (fixed bias) does not work?

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (6/29)

Changes in BJT β changes the bias point drastically. o BJT can end up in saturation or in cut-off easily.

In fixed bias, IB is set through

BJT β then sets IC = β IB (IC changes with β ). o CE circuit then sets VCE .

But, requirements for BJT in active are on IC and VCE and NOT on IB o IC > 0 , VCE > VD0

To make bias point independent of changes in β, the bias circuit should “set” IC and NOT IB !

B

DBBB R

VVI 0 −=

Biasing with Emitter Degeneration

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (7/29)

+

+=−

++=−

EB

EDBB

EEBEBBBB

RRIVV

RIVRIV

1

:KVLBE

0 β

Requires a resistor in the emitter circuit!

EB RR )1( :If +<< β

E

DBBEC

EEDBB

RVVII

RIVV

0

0

≈≈

≈−

Condition of means that the voltage drop across RB is small and the bias voltage VBB – VD0 appears across RE , setting IE and IC ≈ IE .

EB RR )1( +<< β

Independent of β !

Note that resistor RB is NOT necessary for good biasing but it may exist due to other considerations.

Emitter resistor provides negative feedback!

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (8/29)

TBE VVB

EEBEBBBB

eI

RIVRIV

/ ∝

++=

Independent of β ! Negative Feedback:

o If IC ≈ IE ↑ (because β ↑) , VBE ↓ IB ↓ IC ≈ IE ↓

o If IC ≈ IE ↓ (because β ↓) , VBE ↑ IB ↑ IC ≈ IE ↑

β BE -KVL BE junction

BE -KVL BE junction β

Requirements for Biasing with Emitter Degeneration

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (9/29)

Requires a resistor in the emitter circuit.

The bias voltage VBB – VD0 should appear across RE to set IE ≈ IC :

1.

o We need to set to ensure

that this condition is always satisfied!

2. VBE ≈ VD0 . In reality, VBE = VD0 ± ∆VBE with ∆VBE ≈ 0.1 V o We need to set or

EEBBBEBB RIRIVV +=−

EBEEBB RRRIRI )1( +<<⇒<< β

)1( min EB RR +<< β

V 1 ≥EE RI

V 0.1 >>EE RI

Emitter Degeneration Bias with a voltage divider

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (10/29)

CCBB

B

VRR

RV

RRR

×+

=

=

21

2

21

||

Real Circuit

Voltage Divider

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (11/29)

Exercise 3: Find the bias point of the BJT (Si BJT with β = 200 and VA = ∞).

mA 84.2 5107.0)1/(1003.5 2.22

2.22 :KVLBE3

=+++×=

++=−

E

EE

EEBEBB

III

RIVRIβ

V 7.0 and 0 V, 7.0: Activein is BJT Assume

≥>= CECBE VIV

V 0.7 V 10.7 5101084.2101082.2 15

51 :KVLCE

0

333

=>=××++××=

++=−−−

DCE

CE

EECECC

VVV

RIVRI

V 22.215k 34k 9.5

k 9.5

k 03.5k 34||k 9.5||

21

2

21

=×+

=×+

=

===

CCBB

B

VRR

RV

RRR

A 14.1)1/( mA 82.2)1/(

µβββ

=+==+×=

EB

EC

IIII

Notes:

1. We need to solve the complete BE-KVL as we do not know if

2. β >> 1 is a good approximation that reduces the amount of work. Answers using β >> 1 approximation:

)1( EB RR +<< β

V 10.7A 14.2 mA, 2.84

==≈≈

CE

BEC

VIII µ

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (12/29)

Step 1: Find RC and RE

k 2.0k 3.0 k 1.0 :Choose

=−==

EC

E

RRR

Exercise 4: Design a BJT bias circuit (emitter degeneration with voltage divider) such that IC = 2.5 mA and VCE = 7.5 V. (VCC = 15 V Si BJT with β ranging from 50 to 200 and VA = ∞).

k 3.0 5.7)(105.2 15

51 :KVLCE3

=+++××=

++=−−

EC

EC

EECECC

RRRR

RIVRI

Free to choose individual values RE & RC (we will see later that amplifier parameters sets the individual values)

Circuit Prototype

Check:

V 1≥EE RI

V 15.210105.2 33 ≥=××= −EE RI

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (13/29)

Step 2: Find RB and VBB Using relative error, ε = 10% Use largest RB (Will see later why)

Exercise 4 (Cont’d): Design a BJT bias circuit (emitter degeneration with voltage divider) such that IC = 25 mA and VCE = 5 V. (VCC = 15 V Si BJT with β ranging from 50 to 200 and VA = ∞).

k 5.1 k 5.1)1( 0.1 )1( minmin =→=+≤→+<< BEBEB RRRRR ββ

V 20.3 10 10 2.5 0.7

33

0 =→××+=+≈

++=

BB-

ECDBB

EEBEBBBB

VRIVVRIVRIV

Step 3: Find R1 and R2

213.015

3.20

k 10.5||

21

2

21

2121

==+

=

=+

==

RRR

VV

RRRRRRR

CC

BB

B

k 6.4

k 23.9213.0

k 10.5

2

1

=

==

R

R

Step 4: Find commercial R values:

RC = 2 k RE = 1 k R1 = 24 k R2 = 6.4 k

Emitter-degeneration bias circuits

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (14/29)

Basic Arrangement EEBEBBBB RIVRIV ++=

Bias with one power supply

(voltage divider)

EEBEBBBB RIVRIV ++=

Bias with two power supplies

EEBEBBEE RIVRIV ++=

EEEEBEBB VRIVRI −++=0

MOS bias with Gate Voltage (Fixed Bias)

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (15/29)

This method is NOT desirable as µnCox (W/L) and Vt are not “well-defined.” Bias point (i.e., ID and VDS) can change drastically due to temperature and/or manufacturing variability. o See S&S Exercise 5.33 (S&S 5th Ed: Exercise 4.19): Changing Vt from 1 to

1.5 V leads to a 75% change in ID.

DDDDDS

tGSoxnD

RIVV

VVL

WCI

−=

−= 2)( 5.0 µ

MOS bias with Source Degeneration (Resistor RS provides negative feedback!)

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (16/29)

Negative Feedback:

o If ID ↑ (because µnCox (W/L) ↑ or Vt ↓ ) VGS ↓ ID ↓

o If ID ↓ (because µnCox (W/L) ↓ or Vt ↑ ) VGS ↑ ID ↑

ID Eq. GS KVL

GS KVL ID Eq.

Feedback is most effective if

SGDDSGGS

GSDS

RVIIRVVVIR

/ 0 ≈⇒=+−>>

2)( 5.0 tGSoxnD

DSGGS

VVL

WCI

IRVV

−=

−=

µ

Source-degeneration bias circuits

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (17/29)

Basic Arrangement SDGSG RIVV +=

Bias with one power supply

(voltage divider)

Bias with two power supplies

SSSDGS VRIV −+=0

SDGSG RIVV += SDGSSS RIVV +=

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (18/29)

Exercise 5: Find the bias point for Vt = 1 V and µnCox (W/L) = 1.0 mA/V2 (Ignore channel-width modulation).

Voltage divider (IG = 0)

V 715)87/()7( =×+=GV

V 1 065

7)105.0(101

7 7 :KVL-GS

5.0

2

234

2

=→=−+

=××++

=+++==

=

OVOVOV

OVOV

DStOV

DSGSG

OVoxnD

VVVVV

IRVVIRVV

VL

WCI µ

V 5 V 1015

15 :KVL-DS

=−==−=

+=

SDDS

DDD

DDD

VVVIRV

VIR

mA 5.0/ V 527

V 21

===−=−=

=+=

SSD

GSGS

OVGS

RVIVVV

VV

Exercise (impact of RS): Prove that if Vt = 1.5 V (50% change), ID = 0.455mA (9% change)

Biasing in ICs

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (19/29)

Resistors take too much space on the chip. So, biasing with emitter or source degeneration are NOT implemented in ICs.

Recall that the goal of a good bias is to ensure that IC and VCE (or ID and VDS for MOS) do not change. One can force IC (or ID for MOS) to be constant using a current source.

Current source forces IE = I

Current source forces ID = I

BJT response to a current source

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (20/29)

1) Current source forces: III EC =≈

3B) VE is set by BE-KVL

EBEBB VVIR 0 ++=

2) IB = IC / β

3A) CCCCC IRVV −=

4) ECCE VVV −=

MOS response to a current source

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (21/29)

1) Current source forces: IID =

3B) GSGSGS VVVV −=−=

2) VGS is set by 2)( 5.0 tGSoxnD VV

LWCI −= µ

3A) DDDDD IRVV −=

4) SDDS VVV −=

Current Mirrors (or Current Steering circuits) are used as current sources for biasing ICs

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (22/29)

Identical BJTs Qref is always in active since

Identical BJTs and vBE,ref = vBE1

o BJTs will have the same iB and the same iC (ignoring Early effect)

0,,

, 0

DrefBErefCE

refC

VVVi

==

>

βC

CBrefCrefiiiiI 22 :KCL , +=+=

/21

1 refref

C II

iI ≈+

==β

For the current mirror to work, Q1 should be in active:

011 DEECCE VVVV ≥+= Since I1 = const. regardless of

VC1 , this is a current source!

An implementation of a BJT Current Mirror

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (23/29)

RVVVII

VVIRV

DEECCref

EEBErefCCref

01

:)Q ( KVL-BE

−+=≈

−+=

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (24/29)

Exercise 6: Find the bias point of Q2 (Si BJT with β = 100 and VA = ∞).

mA 4.65

mA 4.65

5 1025

1

3

=≈

=

−+×=

ref

ref

BEref

III

VI

Current Mirror

V 1.165 7.0105.4610100

10100 :KVL-BE2

21

263

2223

−==++×××=

++×=−

EC

E

EBEB

VVV

VVI

A 46.5/mA 4.65

22

122

µβ ≈=≈=≈

CB

EC

IIIII

V 7.0 1.56 V 1.56

165.11065.4105

105 :KVL-CE2

02

2

332

2223

=>==

−××−=

++=−

DCE

CE

CE

ECEC

VVVV

VVI

Assume Q2 in active:

Q2 in active!

Check Q1 in active:

V 7.0 3.835V 3.835 5 1.165)5(

01

11

=>==+−=−−=

DCE

CCE

VVVV

Examples of BJT current mirrors

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (25/29)

PNP current Mirror One “reference” BJT feeds many current mirrors

Integer multiple of Iref can be made (See Q3 & Q4)

MOS Current-Steering Circuit

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (26/29)

Qref is always in saturation since

OVOVrefOV

GSGSrefGS

trefGSrefGSrefDS

VVVVVV

VVVV

==

==

−>=

1,

1,

,,,

2111

2,

)/(5.0

)/(5.0

OVoxnD

OVrefoxnrefDref

VLWCiI

VLWCiI

µ

µ

==

==

( )( )refref LW

LWII

// 11 =

For the current steering circuit to work, Q1 should be in saturation:

tGSOVDS VVVV −=>1

Identical MOS: Same µCox and Vt

Since I1 = const. regardless of VD1 , this is a current source!

An implementation of a MOS current steering circuit

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (27/29)

The above quadratic equation gives VOV . I1 is then found from the MOS iD equation.

SSGSDDDref

OVrefoxnDref

VvRiVVLWCiI

−+=

==

:)Q ( KVL-GS

)/(5.0 2µ

0] [ ] )/(5.0 [

02 =+−−++

=+−−+

tDDSSOVOVrefoxn

tDDSSOVD

VVVVVRLWCVVVVRi

µ

Examples of MOS current steering circuits

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (28/29)

One “reference” MOS feeds many current steering circuits.

Any value of Iref can be made (thus, current-steering circuit instead of current-mirror)

( )( )refref LW

LWII

/ / 11 = ( )

( )refref LWLW

II

/ / 22 =

PMOS current steering circuit

An implementation of current steering circuit to bias several transistors in an IC

F. Najmabadi, ECE65, Winter 2013, Amplifier Biasing (29/29)

Exercise: Compute I4/Iref

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