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•Proper biasing circuit which it operate in linear region and circuit have centered Q-point or midpoint biased •Improper biasing cause Improper biasing cause •„Distortion in the output s

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Chapter 4

BJT BIASING CIRCUIT

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Introduction – Biasing

The analysis or design of a transistor amplifier requires knowledge of both the

dc and ac response of the system In fact, the amplifier increases the strength

of a weak signal by transferring the energy from the applied DC source to the weak input ac signal The analysis or design of any electronic amplifier therefore has two components:

•The dc portion and

•The ac portion

During the design stage, the choice of parameters for the required dc levels will affect the ac response

What is biasing circuit?

Biasing: Application of dc voltages to establish a fixed level of current and

voltage

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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

•Proper biasing circuit which it operate in linear region and circuit

have centered Q-point or midpoint biased

•Improper biasing cause Improper biasing cause

•„Distortion in the output signal

•„Produce limited or clipped at output signal

Important basic relationship

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Operating Point

•Active or Linear Region Operation

Base – Emitter junction is forward biased Base – Collector junction is reverse biased Good operating point

•Saturation Region Operation

Base – Emitter junction is forward biased Base – Collector junction is forward biased

•Cutoff Region Operation

Base – Emitter junction is reverse biased

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BJT Analysis

DC analysis

Calculate the DC Q-point

solving input and

output loops

Graphical Method

AC analysis

Calculate gains of the amplifier

DC Biasing Circuits

•Fixed-bias circuit

•Emitter-stabilized bias circuit

•Collector-emitter loop

•Voltage divider bias circuit

•DC bias with voltage feedback

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FIXED BIAS CIRCUIT

configuration

replace them with an open circuit

which;

BE loop (input loop)

CE loop(output loop)

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FIXED BIAS CIRCUIT

circuit

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FIXED BIAS CIRCUIT

1

2

BE Loop CE Loop

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FIXED BIAS CIRCUIT

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FIXED BIAS CIRCUIT

DC C

R

VV

Note that does not affect the value of IcR C

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FIXED BIAS CIRCUIT

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Load line analysis

 A fixed bias circuit with given

values of VCC,RC and RB can be

analyzed ( means,

determining the values of IBQ,

ICQ and VCEQ) using the concept

of load line also.

 Here the input loop KVL

equation is not used for the

purpose of analysis, instead,

the output characteristics of

the transistor used in the

given circuit and output loop

KVL equation are made use

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Plot load line equation

I C(sat) occurs when transistor operating in

CC C

R

V I

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Circuit Values Affect the Q -Point

Decreasing Vcc

Increasing Rc

Varying Ib

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EMITTER-STABILIZED BIAS CIRCUIT

added to improve stability

replace them with an open circuit

which;

BE loop

CE loop

Resistor, R E added

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EMITTER-STABILIZED BIAS CIRCUIT

circuit

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EMITTER-STABILIZED BIAS CIRCUIT

BE Loop CE Loop

1

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EMITTER-STABILIZED BIAS CIRCUIT

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EMITTER-STABILIZED BIAS CIRCUIT

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Improved Bias Stability

The addition of the emitter resistor to the dc bias of the BJT provides improved stability, that is, the dc bias currents and voltages remain closer to where they were set by the circuit when outside conditions, such as temperature, and

transistor beta, change

CC BE c

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VOLTAGE DIVIDER BIAS CIRCUIT

 Provides good Q-point stability with a single polarity supply voltage

beta

VCEQ almost same, thus maintaining the stability of Q point

Exact method : can be applied to any voltage divider circuit

Approximate method : direct method, saves time and energy,

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VOLTAGE DIVIDER BIAS CIRCUIT

Simplified Circuit

Thevenin Theorem;

■ 2nd step: : Simplified circuit using Thevenin Theorem

2 1

2 1

2

1 //

R R

R R

R R

R V

2 1

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VOLTAGE DIVIDER BIAS CIRCUIT

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VOLTAGE DIVIDER BIAS CIRCUIT

RTH E

V V I

ββ

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VOLTAGE DIVIDER BIAS CIRCUIT

CE V I R R

2

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Thus R1 and R2 can be considered as in series.

Voltage divider can be applied to find the voltage across R2 ( VB)

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Approximate Analysis

Then I B << I 2 and I 1 ≅ I 2 : When βR E > 10R 2 ,

From Kirchhoff’s voltage law:

2 1

CC

2 B

R R

V

R V

+

=

E

E E

R

V

I =

BE B

E V V

E E C

C CC

CE V I R I R

) R (R

I V

V

I

I

E C

C CC

independent of any variations in β.

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DC Bias with Voltage Feedback

In this bias circuit

the Q-point is only

slightly dependent on

the transistor beta, β

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Base-Emitter Loop

) R (R

R

V V

I

E C

B

BE CC

I C

I C I' = + ≅

Knowing I C = βI B and I E ≅ I C , the loop

equation becomes:

0 R

I V

R I R

I –

V CC β B CB BBE − β B E =

Solving for I B :

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