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Chapter 4 - Ele232 [Compatibility Mode]

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  • 8/13/2019 Chapter 4 - Ele232 [Compatibility Mode]

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    Chapter : DC Analysis of BJTNorsabrina Sihab

    Faculty of Electrical Engineering,

    Universiti Teknologi MARA

    Pulau Pinang

    Tel : 04-3823355

    . . .

    1

    Chapter 4 DC Analysis of BJT2

    At the end of this chapter, students able to: Analyze the dc biasing of single stage BJT amplifier circuit.

    Calculates DC volta es and DC currents.

    Calculates maximum output voltage, VO(max).

    Electronics 1Updated May 2011NorsabrinaSihab

    Chapter 4 DC Analysis of BJT3

    BiasingBiasing refers to the DC voltages applied to a transistor in order toturn it on so t at it can amp i y t e AC signa .

    The DC input establishes an operating or quiescent point called the

    QQ--pointpoint.In DC analysis all capacitor act as open circuit.

    DC Biasing circuits

    1. Fixed-bias circuit

    2. Emitter-stabilized bias circuit

    3. Voltage divider bias circuit

    Electronics 1Updated May 2011Norsabrina Sihab

    .

    5. Voltage feedback

    Chapter 4 DC Analysis of BJT4

    Proper biasing circuit which it operate in linear region and circuithave centered Q-point or midpoint biased

    mproper as ng cause

    Distortion in the output signal

    Produce limited or clipped at output signali o

    A

    Linear operation for an inverting amplifier

    Electronics 1Updated May 2011NorsabrinaSihab

    Non-linear operation for an inverting amplifier

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    Chapter 4 DC Analysis of BJT5

    -

    Electronics 1Updated May 2011Norsabrina Sihab

    Chapter 4 DC Analysis of BJT6

    1) Fixed-bias circuit - DC analysis

    Input LoopInput Loop Output LoopOutput Loop

    12

    KVL at loop 1: The collector current is given by:

    Solving for the base current:

    CC B B BE =

    KVL at loop 2 :

    )2(= BIIC

    Electronics 1Updated May 2011NorsabrinaSihab

    )1(R

    VVI

    B

    BECCB

    =

    )3(=

    =

    CCCCCE

    CECCCC

    RIVV

    Chapter 4 DC Analysis of BJT7

    Load Line for FixedLoad Line for Fixed--bias circuitbias circuit

    )3(= RIVV

    From equation (3) :

    The end points of the load line

    are:

    VVC

    CC

    satC

    CE

    R

    VI

    0=

    =

    AICCsatCE CVV

    0==

    where the value of RBB sets the value of IBB

    he Q-point is the particular operating point:

    Electronics 1Updated May 2011Norsabrina Sihab

    that sets the values of VCECE and ICC

    Chapter 4 DC Analysis of BJT8

    Circuit Values Affect the QCircuit Values Affect the Q--PointPoint

    Increasing level of IB

    Increasing level of RC

    Decreasingvalue of V

    Electronics 1Updated May 2011NorsabrinaSihab

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    Chapter 4 DC Analysis of BJT9

    -

    Example : Q point at midway between cut-off and saturation

    Csat

    ICQQ-point

    Electronics 1Updated May 2011Norsabrina Sihab

    CE(Cut-off)CEQ

    Chapter 4 DC Analysis of BJT10

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

    Electronics 1Updated May 2011NorsabrinaSihab

    Chapter 4 DC Analysis of BJT11

    2) Emitter2) Emitter--Stabilized Bias CircuitStabilized Bias Circuit

    Adding a resistor (RE) to improve the stability that is DC biascurrent and voltage remain closer to where they set eventemperature c ange.

    Electronics 1Updated May 2011Norsabrina Sihab

    Chapter 4 DC Analysis of BJT12

    2) Emitter2) Emitter--Stabilized Bias CircuitStabilized Bias Circuit DC AnalysisDC Analysis

    npu oopnpu oop u pu oopu pu oop

    KVL at loop 1 :

    1 2

    0RI-V-RI- EEBEBBCC =+V

    Since I = (+1)I :

    KVL at loop 2 :

    0RIVRIV EECECCCC =+

    0R1)I(-RI-V EBBBCC =+ BEV

    Solving for IB:

    E C

    -(2)-)R(RIVV ECCCCCE +=

    Also: EEE RIV =

    Electronics 1Updated May 2011NorsabrinaSihab

    )1(1)R(R

    V-VI

    EB

    BECCB

    ++=

    EBEBBCCB

    CCCCECEC

    VVRIVV

    RI-VVVV

    +==

    =+=

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    Chapter 4 DC Analysis of BJT13

    Load Line for EmitterLoad Line for Emitter--bias circuitbias circuit

    From equation (2) :

    -(2)-)R(RIVV ECCCCCE +=

    The end points of the load lineare:

    VVEC

    CCC

    CE

    sat RR

    VI

    0=+

    =

    AICCCE CVV

    0==

    Electronics 1Updated May 2011Norsabrina Sihab

    Chapter 4 DC Analysis of BJT14

    Determine a) IB, b) IC, c) VCE, d) VC, e) VE, f) VB, g) VBC

    Electronics 1Updated May 2011NorsabrinaSihab

    Chapter 4 DC Analysis of BJT15

    3) Voltage Divider Bias3) Voltage Divider Bias

    This is a very stable.

    The currents and

    independent ofvariations in .

    There are two waysof analyzing thevoltage divider biascircuit :-1. Exact analysis2. Approximate

    Electronics 1Updated May 2011Norsabrina Sihab

    ana ys s

    Chapter 4 DC Analysis of BJT16

    3a) Exact Analysis

    Step 1 : Redraw circuit Step 3 : Replace thevenin equiv.circuit

    BEThB

    VVI

    =

    . ep : pp y o e erm ne Band VCE

    ETh ++

    ( )ECCCCCE RRIVV +=

    Electronics 1Updated May 2011NorsabrinaSihab

    21RRRTh=21

    2

    2 RRVV CCRTh

    +==

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    Chapter 4 DC Analysis of BJT17

    Determine VCE and IC

    Electronics 1Updated May 2011Norsabrina Sihab

    Chapter 4 DC Analysis of BJT18

    Used for circuit that have a very smallIB due to large resistance between

    .

    If Ri R2, IB < I2. So approx. I1 I2

    E 2.

    21

    CC2B

    RR

    VRV

    =

    V

    BEBE VVV

    EE

    RI =

    EECCCCCE RI-RI-VV =

    II CE

    Electronics 1Updated May 2011NorsabrinaSihab

    )R(R-IVV ECCCCCE

    Chapter 4 DC Analysis of BJT19

    Determine VCE and IC

    Electronics 1Updated May 2011Norsabrina Sihab

    Chapter 4 DC Analysis of BJT20

    4) DC Bias with Voltage Feedback

    Another way toimprove the stabilityof a bias circuit is toadd a feedback pathfrom collector tobase.

    In this bias circuitthe Q-point is only

    on the transistor

    beta, .

    Electronics 1Updated May 2011NorsabrinaSihab

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    Chapter 4 DC Analysis of BJT21

    KVL at input loop:

    0= EEBEBBCCCC RIVRIRIV

    B C, .

    CBCC IIII += EC II

    Knowing IC = IB and IE IC, theloop equation becomes:

    = 1

    VV

    EBBEBBCBCC

    Solving for IB:

    Electronics 1Updated May 2011Norsabrina Sihab

    )R(RRI

    ECB

    B++

    =

    Chapter 4 DC Analysis of BJT22

    KVL at output loop:IERE + VCE + ICRC VCC = 0

    Since IC IC as IB=0 and IC = IB:I (R + R ) + V V =0

    Solving for VCE:

    VCE = VCC IC(RC + RE)

    Electronics 1Updated May 2011NorsabrinaSihab

    Chapter 4 DC Analysis of BJT23

    Determine IB and VC

    Electronics 1Updated May 2011Norsabrina Sihab

    Chapter 4 DC Analysis of BJT24

    1) COLLECTOR FEEDBACK

    Determine ICQ, VCEQ, VB, VC, VE and VBC

    Vcc = +20V

    CB

    B2

    Vo

    Electronics 1Updated May 2011NorsabrinaSihab

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    Chapter 4 DC Analysis of BJT25

    2) Common Collector

    Determine VCEQ and IE

    Electronics 1Updated May 2011Norsabrina Sihab

    Chapter 4 DC Analysis of BJT26

    3) Common Base

    Determine VCB, IB and VCE

    CB Co

    VoVi

    E C

    EE CC

    Electronics 1Updated May 2011NorsabrinaSihab

    Chapter 4 DC Analysis of BJT

    27

    Electronics 1Updated May 2011Norsabrina Sihab


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