Chapter 5 Transistors BJT Part I

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    Bipolar Junction Transistors

    The bipolar junction transistor (BJT) is constructedwith three doped semiconductor regions called emitter,base, and collector. These three regions are separated bytwopnjunctions: The base-emitter junction and thebase-collector junction.

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    Transport Model for the npnTransistor

    Base-emitter voltage vBEand base-collector voltage vBCdetermine currents intransistor and are said to be positive when they forward-bias their respective

    pnjunctions.

    The terminal currents are collector current(iC), base current (iB) and emitter

    current (iE).

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    npn Transistor | Forward Characteristics

    Collector (Forward transport) current

    is

    ISis the BJT saturation current

    Base current iB is given by

    bF is the forward common-emitter current gain

    Emitter current iE is

    aF is the forward common-base current gain

    In this forward-active region of operation

    195.0

    11exp

    F

    F

    FF

    T

    BE

    F

    SBCE

    V

    vIiii

    a

    b

    ba

    a

    E

    CF

    B

    CF

    i

    i

    i

    i ab

    VT= kT/q =0.025 V at room temperature

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    Emitter current iE is

    1expT

    BCSRE

    V

    vIii

    1exp

    T

    BC

    R

    S

    R

    RB V

    vIii

    bb

    Collector current iC is given by

    bRis the reverse common-emitter current

    gain

    aRis the reverse common-base current gain

    Base current iB is given by

    Base currents in forward and reverse modes

    are different due to asymmetric doping levels

    in emitter and collector regions.

    95.001

    R

    ab

    ba

    R

    RR

    npn Transistor | Reverse Characteristics

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    First term in both emitter and collector current expressions gives current transported

    completely across base region.

    npn Transistor | Complete Transport ModelEquations for Any Bias

    1exp1exp

    1expexpexp

    1expexpexp

    T

    BC

    R

    S

    T

    BE

    F

    SB

    T

    BE

    F

    S

    T

    BC

    T

    BE

    SE

    T

    BC

    R

    S

    T

    BC

    T

    BESC

    V

    vI

    V

    vIi

    V

    vI

    V

    v

    V

    v

    Ii

    VvI

    Vv

    VvIi

    bb

    b

    b

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    Transport Model Calculation| Example

    Problem: Find terminal voltages and currents. Given data: VBB = 0.75 V, VCC= 5.0 V, IS = 10

    -16 A,

    bF= 50,bR = 1

    Assumptions: Room temperature operation, VT= 25.0 mV.

    Analysis: VBE= 0.75 V,

    VBC= VBB -VCC= 0.75 V- 5.00V = - 4.25 V

    AI

    mAI

    mAI

    B

    E

    C

    4.211

    025.0

    25.4exp

    1

    101

    025.0

    75.0exp

    50

    10

    09.11025.0

    75.0exp

    50

    10

    025.0

    25.4exp

    025.0

    75.0exp10

    07.11

    025.0

    25.4exp

    1

    10

    025.0

    25.4exp

    025.0

    75.0exp10

    1616

    1616

    1616

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    i-v Characteristics of Bipolar Transistors

    1. Common-

    Emitter Output

    Characteristics

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    i-v Characteristics of Bipolar TransistorsCommon-Emitter Output Characteristics

    For iB = 0, the transistor is cutoff. If iB > 0, iCalso increases.

    For vCE> vBE, npn transistor is in forward-active region, iC = bFiB is nearlyindependent of vCE.For vCE< vBE, transistor is in saturation.

    For vCE< 0, roles of collector and emitter reverse.

    Three regions are recognized

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    Operation Regions of BipolarTransistors

    Base-Emitter Junction Base-Collector Junction

    Reverse Bias Forward Bias

    Forward Bias

    Forward-Active

    Region(Good Amplifier)

    Saturation Region

    (Closed Switch)

    Reverse BiasCutoff Region

    (Open Switch)

    Reverse-Active

    Region

    (Poor Amplifier)

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    i-v Characteristics of Bipolar Transistors

    2. Transfer Characteristics

    Defines relation between collector

    current and base-emitter voltage of

    transistor.

    Almost identical to transfer

    characteristic of apnjunction diode

    Setting vBC = 0 in the collector-current

    expression yields

    Collector current expression has the same form as that of the diode equation

    1exp

    T

    BESC

    VvIi

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    Simplified Cutoff Region Model

    In the cutoff region, both junctions

    are reverse-biased; the transistor is

    said to be in off state

    vBE< 0, vBC< 0

    If we assume that

    where 4kT/q = 0.1 V, then the

    transport model terminal current

    equations simplify to

    q

    kTv

    q

    kTv BCBE 4and4

    F

    S

    F

    SB

    F

    SE

    R

    SC

    IIi

    IiIi

    bb

    bb

    and

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    Simplified Cutoff Region ModelExample

    Problem: Estimate terminal currents using the transport model

    Given data: IS = 10-16 A, aF= 0.95, aR = 0.25, VBE= 0 V, VBC= -5 V

    Assumptions: Simplified transport model assumptions

    Analysis: From given voltages, we know that transistor is in cutoff.

    For practical purposes, all three

    currents are essentially zero.

    AxII

    AII

    AxI

    II

    R

    SB

    SE

    R

    S

    R

    SC

    16

    16

    16

    103

    10

    1041

    1

    b

    ab

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    Simplified Forward-Active RegionModel

    In forward-active region, the emitter-base junction is forward-biased and thecollector-base junction is reverse-biased. vBE > 0, vBC< 0. if we assume

    then the transport model terminal current equations simplify to

    BJT is often considered a current-controlled device, though fundamental

    forward-active behavior suggests a voltage- controlled current source.

    1expexp

    expexp

    exp

    BFB

    T

    BE

    F

    S

    R

    S

    T

    BE

    F

    SB

    BFC

    T

    BE

    F

    S

    F

    S

    T

    BESE

    EFC

    R

    S

    T

    BESC

    IiV

    vII

    V

    vIi

    Ii

    V

    vII

    V

    vIi

    IiI

    V

    vIi

    bbbb

    b

    ab

    ab

    q

    kTv

    q

    kTv BCBE 4and4

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    Simplified Forward-Active RegionModel | Example 1

    Problem: Estimate transistor terminal currents and base-emitter voltage

    Given data:IS=10-16 A,aF= 0.95, VBC= VB - VC = -5 V,IE= 100 A

    Assumptions: Simplified transport model assumptions, room

    temperature operation, VT = 25.0 mV

    Analysis: Current source forward-biases base-emitter diode, VBE> 0,

    VBC< 0, we know that transistor is in forward-active operation region.

    VI

    IVV

    AAI

    I

    AAII

    S

    EFTBE

    F

    EB

    F

    FF

    EFC

    689.0ln

    520

    100

    1

    1995.01

    95.0

    1

    9510095.0

    a

    b

    a

    ab

    a

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    Problem: Estimate terminal currents, base-emitter and base-collectorvoltages for the transistor in the given circuit.

    Given data:IS= 10-16 A,aF= 0.95, VC = +5 V,IB = 100 A

    Assumptions: Simplified transport model assumptions, room

    temperature operation, VT = 25.0 mV

    Analysis: Current source causes base current to forward-bias base-emitter diode, VBE> 0, VBC

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    Simplified Circuit ModelForward-Active Region

    Current in base-emitter diode is amplified by common-emitter current gain

    bFand appears at collector; base and collector currents are exponentiallyrelated to base-emitter voltage.

    Base-emitter diode is replaced by constant voltage drop model (VBE= 0.7 V)since it is forward-biased in forward-active region.

    dc base and emitter voltages differ by 0.7-V diode voltage drop in forward-active region.

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    Simplified Forward-Active RegionModel | Example 3

    Problem: Find transistor Q-point Given data: bF= 50, bR = 1

    Assumptions: Forward-active region of operation, VBE = 0.7 V

    Analysis:

    correct.isregionactive-Forward

    44.57.03.499.09

    m990.08.1950

    8.1951

    01.1

    1

    01.18200

    7.09

    08200

    VKmAV

    VRIVV

    AAII

    AmAI

    I

    mAV

    I

    VIV

    CE

    BECCCCCE

    BFC

    F

    EB

    E

    EEEBE

    b

    b

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    Simplified Circuit ModelSaturation Region

    In the saturation region, both junctions are forward-biased, and thetransistor operates with a small voltage between collector and emitter.vCESAT is the saturation voltage for the npn BJT.

    No simplified expressions exist for

    terminal currents other than iC+ iB = iE.

    Simplified Model

    F

    CB

    BF

    C

    BR

    C

    R

    TBCBECESAT

    T

    BC

    R

    S

    T

    BE

    F

    SB

    T

    BC

    R

    S

    T

    BESC

    II

    I

    I

    I

    I

    VVVV

    V

    VI

    V

    VII

    V

    VI

    V

    VII

    b

    b

    b

    a

    bba

    for

    1

    11

    1ln

    expexpexpexp

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    Transconductance Transconductance is defined by:

    T

    C

    PtQT

    BES

    BEPtQBE

    Cm

    V

    I

    V

    vI

    dv

    d

    dv

    dig

    exp

    Biasing for the BJT The goal of biasing is to establish known Q-point which in turn establishes

    initial operating region of the transistor.

    For a BJT, the Q-point is represented by (IC, VCE) for an npn transistor or (IC, VEC)

    for apnp transistor.

    Two practical biasing circuits used for a BJT are:

    Four-Resistor Bias Network

    Two-Resistor Bias Network