Biasing the BJT

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    Biasing the BJT

    To operate as an amplifier a transistor must be biased in

    the active region

    The transistor, when properly biased can amplify a small

    ac signal faithfully

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    Transistor Circuit

    under D. C. Condition

    Transistor Circuit withA. C. Signal at input

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    iB= IB+ IbiE = IE+ ieiC = IC+ ic

    IB, IC,IE - D.C. currentsIb, ic, ie A.C. currents

    iB, iC, iE D.C + A.C. currents

    Similarly,

    VBE, VCE D.C. Voltages

    vbe, vce A.C.VoltagesvBE, vCE D.C+ A.C Voltages

    Transistor Circuit with A. C. Signal

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    vCE = VCC- iCRC= VCC - (IC+ ic)RC= VCC- ICRC - icRC= VCE icRC

    VCE = D.C. Bias voltage at

    the collector

    Considering only the A. C. Voltage at the collector,

    vo= vce = - icRC

    Voltage gain = vo/vi

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    VBE =VBB IBRB

    Transistor Circuit under D. C. Condition

    VBB/RB

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    VCE =VCC- ICRCWhen IC = 0, VCE =VCCWhen VCE = 0, IC =VCC/RC

    VCC/RC

    Q is the operating point

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    Operating Point or Quiscent Point

    The intersection of the load line with the transistoroutput characteristic for a particular IB gives the

    operating point Q(VCEQ, ICEQ)

    VCC/RC

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    Effect of Q-point location on allowable signal swing

    Load- line A results in an

    operatingpoint too close to the

    cut-off region and thus limits

    the positive swing ofvCE

    Load-line B results in an

    operatingpoint too close to the

    saturation region and thus limits

    the negative swing of vCE

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    Selection ofOperating Point Q

    A good selection of the operatingpoint Q is essential inorder that an amplifier circuit amplifies an A.C signal

    without any distortion

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    BiasingMethods

    1. Fixed Bias

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    Fixed Bias Circuit

    D.C. EquivalentC1 and C2 open circuit under D.C.

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    Using KVL in the base-emitter loop,

    VCC IBRBVBE = 0

    or, IB = (VCC-VBE)/RB

    IC = IB=(VCC-VBE)/RB

    Using KVL in the collector-emitter

    loop,

    VCC ICRCVCE = 0

    or, VCE = VCC - ICRCQ(VCE,IC) is set

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    2. Emitter and Collector Feedback Bias

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    Emitter and Collector Feedback Bias

    D.C. EquivalentApplying KVL

    or, VCC- (IC+IB)RC- IBRB-VBE-(+1)IBRE= 0

    or, VCC- (IB+IB)RC- IBRB-VBE- (+1)IBRE = 0or, VCC {RB+(+1) (RC+RE)}IB-VBE = 0

    or, )R(R1RVV

    IECB

    BECC

    B

    ! VCE = VCC- (IC+IB)(RC+RE)

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    BiasS

    tabilization

    )(1)(

    I

    If RB

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    3. Voltage Divider Bias

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    D.C. EquivalentVoltage Divider Bias

    IR1

    IR2 IB

    IC

    IE

    Ignoring IB(as very small), IR1 = IR2We can use Thevenins Theorem

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    Thevenins Equivalent Circuit

    for the base-emitter loop

    )( 21

    2

    Th

    !

    )( 21

    21

    21Th

    !!

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    Base-Emitter Loop

    ETh

    BEThB

    EBBEThBTh

    R1R

    VVIor,

    0RI1VRIV

    !

    !

    Collector- Emitter Loop

    ETh

    BEThBC

    R1R

    )V(VII

    !!

    EBCCCCCEECCCCCE )RI(IRIVRIRIVV !!

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    Bias Stabilization

    ETh

    ETh

    1)(I

    !

    If RTh

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    Ex.1

    Fig.1

    For the circuit shown in Fig.1,

    find the change in IC when

    changes from 100 to 300.