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BFF1303: ELECTRICAL / ELECTRONICS ENGINEERING Analog Electronics: BJT Biasing Circuits Ismail Mohd Khairuddin , Zulkifil Md Yusof Faculty of Manufacturing Engineering Universiti Malaysia Pahang

BFF1303: ELECTRICAL / ELECTRONICS ENGINEERING Analog

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BFF1303: ELECTRICAL /

ELECTRONICS ENGINEERING

Analog Electronics:

BJT Biasing Circuits

Ismail Mohd Khairuddin , Zulkifil Md Yusof

Faculty of Manufacturing Engineering Universiti Malaysia Pahang

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 2

Faculty of Manufacturing Universiti Malaysia Pahang

Kampus Pekan, Pahang Darul Makmur Tel: +609-424 5800 Fax: +609-4245888

http://fkp.ump.edu.my/

Bipolar Junction

Transistor-DC Biasing

BFF1303 ELECTRICAL/ELECTRONICS ENGINEERING

Contents:

Outcomes

Operating Point

Fixed-Bias Circuit

Emitter Bias

Voltage-Divider Bias

DC Bias with Voltage Feedback

Design Operations

Transistor Switching Network

PNP Transistor

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BFF1303 Electrical/Electronic Engineering 3

Understand the physical operation of bipolar

transistor

Select the operating point of a bipolar transistor circuit

Compute performance of several important

amplifier configurations.

Select an amplifier configuration appropriate

for a given application.

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BFF1303 Electrical/Electronic Engineering 4

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

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

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BFF1303 Electrical/Electronic Engineering 5

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

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BFF1303 Electrical/Electronic Engineering 6

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Base-Emitter Loop

From Kirchhoff’s voltage law:

Solving for base current:

+VCC – IBRB – VBE = 0

CC BEB

B

V VI

R

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BFF1303 Electrical/Electronic Engineering 8

Collector-Emitter Loop

Collector current:

From Kirchhoff’s voltage law:

C BI I

CE CC C CV V I R

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BFF1303 Electrical/Electronic Engineering 9

240k

2.2k

12V

10 F

10 F

50

Determine the following for the fixed-bias configuration of figure shown

, , , , ,B C CE B C BCI I V V V V

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BFF1303 Electrical/Electronic Engineering 10

Solution

Apply KVL to Base-Emitter loop,

0CC B B BEV R I V

Then CC BEB

B

V VI

R

12 0.747.08 A

240kBI

Collector current:

2.35mAC BI I

Apply KVL to Collector-Emitter loop,

6.83V

CE CC C C

CE

V V I R

V

0.7 V

6.83V

B BE

C CE

V V

V V

6.13V

BC B C

BC

V V V

V

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BFF1303 Electrical/Electronic Engineering 11

The dc bias circuit shown in figure below has RB = 200 kΩ , RC = 1 kΩ, and VCC = 15V. The transistor β has = 100. Solve for IC and VCE

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BFF1303 Electrical/Electronic Engineering 12

Solution

Apply KVL to Base-Emitter loop,

0CC B B BEV R I V

CC BEB

B

V VI

R

15 0.771.5 A

200kBI

Collector current:

100 71.5

7.15mA

C B

C

C

I I

I

I

Apply KVL to Collector-Emitter loop,

15 7.15 1k 7.85V

CE CC C C

CE

V V I R

V

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BFF1303 Electrical/Electronic Engineering 13

Transistor Saturation

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

sat

CCC

C

VI

R 0 VCEV

Actual Approximate

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BFF1303 Electrical/Electronic Engineering 14

Load-Line Analysis

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Load-Line Analysis

ICsat

IC = VCC / RC

VCE = 0 V

VCEcutoff

VCE = VCC

IC = 0 mA

where the value of RB sets the value of IB

that sets the values of VCE and IC

The Q-point is the operating point:

The end points of the load line are:

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Circuit Values Affect the Q-Point

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Circuit Values Affect the Q-Point

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

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Base-Emitter Loop

From Kirchhoff’s voltage law:

( 1) 0CC B B B EV I R I R

0CC B B BE E EV I R V I R

( 1)

CC BEB

B E

V VI

R R

Since IE = (β + 1)IB:

Solving for IB:

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BFF1303 Electrical/Electronic Engineering 20

Collector-Emitter Loop

From Kirchhoff’s voltage law:

CE CC C C EV V I R R

0E E CE C C CCI R V I R V

E E E

C CE E CC C C

B CC R B BE E

V I R

V V V V I R

V V I R V V

Since IE IC :

Also:

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BFF1303 Electrical/Electronic Engineering 21

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

The endpoints can be determined from the load line.

VCEcutoff : ICsat:

0 mA

CE CC

C

V V

I

0 VCE

CCC

C E

V

VI

R R

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BFF1303 Electrical/Electronic Engineering 22

This is a very stable bias circuit.

The currents and voltages are nearly independent of any variations in β.

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BFF1303 Electrical/Electronic Engineering 23

Approximate Analysis

Where IB << I1 and I1 I2 :

Where βRE > 10R2:

From Kirchhoff’s voltage law:

2

1 2

CCB

R VV

R R

EE

E

E B BE

VI

R

V V V

CE CC C C E EV V I R I R ( )

E C

CE CC C C E

I I

V V I R R

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BFF1303 Electrical/Electronic Engineering 24

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.

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Base-Emitter Loop

( )

CC BEB

B C E

V VI

R R R

From Kirchhoff’s voltage law:

' – – – – 0CC C C B B BE E EV I R I R V I R

Where IB << IC:

'

C C B CI I I I

Knowing IC = IB and IE IC, the loop equation becomes:

– 0CC B C B B BE B EV I R I R V I R

Solving for IB:

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Base-Emitter Bias Analysis

Transistor Saturation Level

EC

CCCmaxCsat

RR

VII

Load Line Analysis

Cutoff: Saturation:

mA 0I

VV

C

CCCE

V 0VCE

ER

CR

CCV

CI

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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.