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Unit 2: Transistor Biasing INTRODUCTION BJTs amplifier requires a knowledge of both the DC analysis (LARGE-signal) and AC analysis (small signal). For a DC analysis a transistor is controlled by a number of factors including the range of possible operating points. Once the desired DC current and voltage levels have been defined, a network must be constructed that will establish the desired operating point. BJT need to be operate in active region used as amplifier. The cutoff and saturation region used as a switches. For the BJTs to be biased in its linear or active operating region the following must be true: BE junction forward biased, 0.6 or 0.7V BC junction reverse biased DC bias analysis assume all capacitors are open cct. AC bias analysis : 1) Neglecting all of DC sources 2) Assume coupling capacitors are short cct. The effect of these capacitors is to set a lower cut- off frequency for the cct. 3) Inspect the cct (replace BJTs with its small signal model). 4) Solve for voltage and current transfer function and i/o and o/p impedances. For transistor amplifiers the resulting DC current and voltage establish an operating point that define the region that can be employed for amplification process. Biasing Biasing: The DC voltages applied to a transistor in order to turn it on so that it can amplify the AC signal.

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Unit 2: Transistor Biasing

INTRODUCTION

BJTs amplifier requires a knowledge of both the DC analysis (LARGE-signal) and AC analysis (small signal).

For a DC analysis a transistor is controlled by a number of factors including the range of possible operating points.

Once the desired DC current and voltage levels have been defined, a network must be constructed that will establish the desired operating point.

BJT need to be operate in active region used as amplifier.

The cutoff and saturation region used as a switches.

For the BJTs to be biased in its linear or active operating region the following must be true:

BE junction forward biased, 0.6 or 0.7V

BC junction reverse biased

DC bias analysis assume all capacitors are open cct.

AC bias analysis :

1) Neglecting all of DC sources

2) Assume coupling capacitors are short cct. The effect of these capacitors is to set a lower cut-off frequency for the cct.

3) Inspect the cct (replace BJTs with its small signal model).

4) Solve for voltage and current transfer function and i/o and o/p impedances.

For transistor amplifiers the resulting DC current and voltage establish an operating point that define the region that can be employed for amplification process.

Biasing

Biasing: The DC voltages applied to a transistor in order to turn it on so that it can amplify the AC signal.

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15

18

12

9

6

3

IC(mA)

VCE(V)

IB=60 uA

10 20 30

IB=50 uA

IB=0 uA

IB=40 uA

IB=30 uA

IB=20 uA

IB=10 uA

40

A

C

B

VCEsat

PCmax

ICmax

VCEmaxCutoff

Saturation

Operating Point

The DC input establishes an operating or quiescent point called the Q-point.

Various operating points within the limits of operation of a transistor

Q-point B:

• The best operating point for linear gain and largest possible voltage and current

• It is a desired condition for a small signal analysis

Q-point A:

• I=0A, V=0V

• Not suitable for transistor to operate

Q-point C:

• Concern on nonlinearities due to IB

• curves is rapidly changes in this region.

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RCRB

+VCC

ic

vceib

v in

v out

The Three States of Operation

• Active or Linear Region Operation

Base–Emitter junction is forward biased

Base–Collector junction is reverse biased

• Cutoff Region Operation

Base–Emitter junction is reverse biased

• Saturation Region Operation

Base–Emitter junction is forward biased

Base–Collector junction is forward biased

DC Biasing Circuits

The ac operation of an amplifier depends on the initial dc values of IB, IC, and VCE. By varying IB around

an initial dc value, IC and VCE are made to vary around their initial dc values. DC biasing is a static

operation since it deals with setting a fixed (steady) level of current (through the device) with a desired

fixed voltage drop across the device.

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RCR1

+VCC

IC

IE

RE

R2

IC(mA)

VCE

VCE(off) = VCC

IC(sat) = VCC/(RC+RE)

DC Load Line

cmxy

RRVV

RRI

IIRIVRIV

EC

CCCE

EC

C

EECECCCC

EC

+=

++

+−

=

≈=−−−

:equation linestraight of form slope-Point

1for

0

Purpose of the DC biasing circuit To turn the device “ON” . To place it in operation in the region of its

characteristic where the device operates most linearly, i.e. to set up the initial dc values of IB, IC, and

VCE

Types

• Fixed-bias circuit

• Emitter-stabilized bias circuit

• Collector-emitter loop

• Voltage divider bias circuit

• DC bias with voltage feedback

Graphical DC Bias Analysis

DC Load Line

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The straight line is know as the DC load line

Its significance is that regardless of the behavior of the transistor, the collector current IC and the

collector-emitter voltage VCE must always lie on the load line, depends ONLY on the VCC, RC and RE

(i.e. The dc load line is a graph that represents all the possible combinations of IC and VCE for a

given amplifier. For every possible value of IC, and amplifier will have a corresponding value of VCE.)

It must be true at the same time as the transistor characteristic. Solve two condition using

simultaneous equation

→ graphically → Q-point !!

Q-Point (Static Operation Point)

When a transistor does not have an ac input, it will have specific dc values of IC and VCE.

These values correspond to a specific point on the dc load line. This point is called the Q-point.

The letter Q corresponds to the word (Latent) quiescent, meaning at rest.

A quiescent amplifier is one that has no ac signal applied and therefore has constant dc values of IC

and VCE.

The intersection of the dc bias value of IB with the dc load line determines the Q-point.

It is desirable to have the Q-point centered on the load line.

Why?

When a circuit is designed to have a centered Q-point, the amplifier is said to be midpoint biased.

Midpoint biasing allows optimum ac operation of the amplifier.

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DC Biasing + AC signal

When an ac signal is applied to the base of the transistor, IC and VCE will both vary around their Q-

point values.

When the Q-point is centered, IC and VCE can both make the maximum possible transitions above and

below their initial dc values.

When the Q-point is above the center on the load line, the input signal may cause the transistor to

saturate. When this happens, a part of the output signal will be clipped off.

When the Q-point is below midpoint on the load line, the input signal may cause the transistor to

cutoff. This can also cause a portion of the output signal to be clipped.

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IC(mA)

VCE

VCE(off) = VCC

IC(sat) = VCC/(RC+RE)

DC Load Line IC

VCE

IC(sat) = ICQ + (VCEQ/rC)

VCE(off) = VCEQ + ICQrC

ac load line

IC

VCE

Q - point

ac load line

dc load line

AC Load Line

• The ac load line of a given amplifier will not follow the plot of the dc load line.

This is due to the dc load of an amplifier is different from the ac load

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AC inputsignal

AC outputsignal

RBRC

BC

EVBE

VCE+

+

--

C1

C2

C1,C2 = coupling capacitors

VCC

IC

IB

RBRC

BC

EVBE

VCE+

+

--

VCC

IC

IB

VCC

What does the ac load line tell you?

The ac load line is used to tell you the maximum possible output voltage swing for a given common-

emitter amplifier.

In other words, the ac load line will tell you the maximum possible peak-to-peak output voltage (Vpp )

from a given amplifier.

This maximum Vpp is referred to as the compliance of the amplifier.

(AC Saturation Current Ic(sat) , AC Cutoff Voltage VCE(off) )

Fixed Bias

AC ANALYSIS DC ANALYSIS

The Base-Emitter Loop

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Collector-Emitter Loop

Saturation

When the transistor is operating in saturation, current through the transistor is at its maximum possible

value.

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Load Line Analysis

The Q-point is the operating point:

• where the value of RB sets the value of IB

• sets the V and I

that values of VCE IC

Circuit values affect the Q point

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Emitter-Stabilized Bias Circuit

Adding a resistor (RE) to the emitter circuit stabilizes the bias circuit.

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Base-Emitter Loop

Collector Emitter Loop

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RCR1

+VCC

RE

R2

v out

v in

C2C1

C3

Improved Biased Stability

Stability refers to a circuit condition in which the currents and voltages will remain fairly

constant over a wide range of temperatures and transistor Beta (β) values. Adding RE to the

emitter improves the stability of a transistor.

Saturation Level

Voltage-Divider Bias

The voltage – divider (or potentiometer) bias circuit is by far the most commonly used.

RB1, RB2 -> voltage-divider to set the value of VB , IB

C3 -> to short circuit ac signals to ground, while not effect the DC operating (or biasing) of a

circuit

(RE stabilizes the ac signals)

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Approximate Analysis

Voltage Divider Bias Analysis

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DC Bias with Voltage Feedback

Another way to improve the stability of a bias circuit is to add a feedback path from collector to

base.

In this bias circuit the Q-point is only slightly dependent on the transistor beta, β.

Base-Emitter Loop

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Collector Emitter Loop

Base Emitter Bias Analysis

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Miscellaneous configuration

Transistor Switching Networks

Transistor works as an inverter in computer circuits.

Operating point switch from cut-off to saturation along the load line for proper inversion.

In order to understand, we assume that;

IC=ICEO=0mA

VCE=Vsat=0V

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One must understand the transistor graph output and load-line analysis to describe and discuss

about the transistor switching networks.

Transistors with only the DC source applied can be used as electronic switches.

Switching Circuit Calculations

Switching Time

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PNP Transistors

The analysis for pnp transistor biasing circuits is the same as that for npn transistor circuits. The

only difference is that the currents are flowing in the opposite direction.

Bias stabilization

• Stability of a system is a measure of the sensitivity of a network to variation in its

parameter.

– β increases with increase in temperature

– VBE decreases 7.5mV every degree celcius

– ICO doubles every 10 oC increase in temperature

Effect of non-stability circuit/system

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E

BCO

E

B

CO

E

B

CO

E

B

E

B

E

B

CO

RRIS

RR

ISR

RIS

RR

RR

RR

IS

+

=

+<<

+=

+>>

++

++=

)(, be lfactor wil

stability 1, to1 from of rangesFor

1)(

toreduce it will ),1( If

)1()(

toreduce it will ),1( If

)()1(

)(1)1()(

β

β

β

β

ββ

ββ

∆∆

=

∆∆

=

∆∆

=

C

BE

CBE

CO

CCO

IS

VIVS

IIIS

)(

)(

)(

We’ll find that β increase after 100OC, base current is same but not suitable

to use due it is very near to the saturation region.

Stability factors

S(ICO)

Emitter bias configuration

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valuemaximum reach the and stablenot sit' so)....1()(obtain, ll we'0R assume andr,denumerato andnumerator for theRith equation w above gmultiplyin If

)()1(

)(1)1()(

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+=Ω=

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β

ββ

CO

E

B

E

B

CO

IS

RR

RR

IS

rule.Thevenin usinganalyze becauseonly differsbut stic,characteri

ionconfigurat bias-emitter the tosame is This

)()1(

)(1)1()(

E

Th

E

Th

CO

RR

RR

IS++

++=

ββ

Ω=

++

++=

0 Where

)()1(

)(1)1()(

E

C

B

C

B

CO

RRR

RR

ISβ

β

• Fixed bias configuration

• Voltage divider bias configuration

• Feedback bias configuration

• Physical impact

Fixed bias configuration ; IC=βIB+(β+1)ICO...IC increase but IB maintain, so it’s not stable

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)1 if(......1

)1(

or

)0R if(......

)1(

)(

E

E

B

E

E

B

E

B

EB

BE

CBE

RR

R

RR

R

R

RR

VIVS

>>+−=

++

=

Ω=−=

++−

=

∆∆

=

β

β

β

ββ

β

)1(

)1(

)(

21E

B

E

BC

C

C

RR

RRI

I

IS

++

++=

∆∆

=

ββ

ββ

Emitter bias configuration ; Increase IC will increase ICO. It affect VE since VE=IERE=ICRE. In turn,

the output loop will inform that IB will decrease if VE is increase, thus affect to reduce the collector

current.

Feedback bias configuration ; same as result of emitter bias configuration where IB will decrease

if IC increase. (IC proportional to VRC)

Voltage divider bias configuration ; Most stable where as long as 10R2>> βRE, VB remain

constant for any changing in IC.

S(VBE) S(β)

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AC inputsignal

AC outputsignal

RC=2.2kohm

BC

EVBE

VCE+

+

--

C1

C2

VCC=+12V

IC

IB

10uF

10uF

RB=240kohm

Fig. 5.3

( )( )

( )( )

biased.reverse isjunction -BC that indicatessign ve-

6.13V83.67.0)

V 6.83VVV

V 0.7VV )

83.62.22.35m-12RI-VV )

34.208.4750I

08.47240

7.012

)

CCEQCE

BBE

CCCCCEQ

CQ

−=−=−=

===

==

==

=

===

=−

=

−=

CBBC

BQ

B

BECCBQ

VVVd

c

Vk

b

mAuI

uAk

RVVIa

β

Example 1:

Determine the following for the fixed bias configuration of Fig 5.3.

a) IBQ and ICQ b) VCEQ c) VB and VC d) VBC

Solution:

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RC=2.7kohm

BC

EVBE

VCE+

+

--

VCC=+16V

IC

IB

RB=470kohm

Fig. 5.4

( )( )

( )( )

VVe

c

Vk

b

mAuI

uAk

RVVIa

E

BQ

B

BECCBQ

0)

V 8.17VVd)V

V 0.7VV )

17.87.22.93m-16RI-VV )

93.255.3290I

55.32470

7.016

)

CCEQCE

BBE

CCCCCEQ

CQ

=

===

==

==

=

===

=−

=

−=

β

Determine the following for the fixed bias configuration of Fig 5.4.

a) IBQ and ICQ b) VCEQ c) VB d)VC e) VE

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RC=560ohm

BC

EVBE

VCE+

+

--

VCC=+12V

IC

IB

RB=100kohm

Fig. 5.11

( )( )

( )( )( )

( )( )

( )( )16.95mA) V, (2.51point -Q New51.2

56016.95m-12RI-V V

:4 Step

mA 16.95113150II

same, is valuetheA 113100k

0.7-12I

150, new :3 Step

3.11,67.5int67.55603.11-12RI-V V

:2 Step

mA 11.3113100II

A 113100k

0.7-12I

100,:1 Step

CCCCCE

BC

B

CCCCCE

BC

B

=

===

⇒==

=

−⇒==

=

===

==

=

V

mAVpoQVm

µβ

µ

β

µβ

µ

β

Example 6:

Determine the value of Q-point for Fig. 5.11. Also find the new value of Q-point if

β change to 150.

The change of β cause the big change of

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Q-point value. This shows that fixed biased configuration is NOT stable