Chapter 1 BJT Amplifier

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    Bipolar Junction Transistor (BJT)

    and Linear Amplifier

    Chapter 1BJT Amplifiers

    1 2013/2014 EKT204

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    Outline

    2013/2014 EKT2042

    IntroductionBJT Linear AmplifierGraphical Analysis & AC Equivalent CircuitSmall-signal hybrid- equivalent circuit

    Hybrid- Equivalent Circuit and Early EffectExpanded Hybrid- Equivalent CircuitAC Load Line AnalysisMaximum Symmetrical Swing Common-emitter AmplifierCommon-collector AmplifierCommon-base Amplifier

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    Introduction

    2013/2014 EKT2043

    Analog Electronic Circuits Analog Electronic Circuits produce ananalog signals

    Linear amplifier circuitMagnifies input signal & produce output

    signal that is larger & directlyproportional to input signalElectronic

    CircuitSignalInput

    SignalOutput

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    BJT Linear AmplifierBJT needs to be biased with DC voltage atquiescent point (Q-point) where BJT is biased inforward active region

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    Linear Amplifier

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    Time-varying output voltage is directlyproportional to & larger than time-varying inputvoltage

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    Graphical Analysis & ACEquivalent Circuit

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    A common -emitter circuit with time-varyingsignal source in series with the base DC source

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    2013/2014 EKT2047

    Graph plots collector current (i c) vs collector-emitter potential (v CE ).For different base currents (i B) different curves are obtained.

    AC base current superimposed on I BQ - time-varying base current inducesac collector current superimposed on I CQ

    AC collector-emitter voltage = output voltage - is larger than the input =amplificationLinear amplifier = ac added / superimposed on dc ==> superposition ==>only if ac is small ==>small signal analysis .

    Line between VCC /R C and V CC = dc load line

    Q-point is chosen wheredistance between i B curves aresimilar / even so thatamplification properties arelinear.

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    Contd time-varying signals linearly related & superimposedon dc values)

    If signal source, v s = 0:

    (4)

    (3) (2)

    (1)

    be BEQ BE

    ceCEQCE

    cCQC

    b BQ B

    vV v

    vV vi I i

    i I i

    (6) loop)E-(C

    (5) loop)E-(B

    CEQC CQCC

    BEQ B BQ BB

    V R I V

    V R I V

    2013/2014 EKT2048

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    Contd For B-E loop, considering time varying signals:

    Rearrange:

    Base on (5), left side of (7) is 0. So:

    For C-E loop, considering time varying signals:

    9Base on (6), left side of (11) is 0. So:

    (7) )()( be BEQ Bb BQ BE B B s BB vV Ri I v RivV

    (8) sbe Bb BEQ B BQ BB vv RiV R I V

    (9) be Bb s v Riv

    (11) (10)

    ceccCEQC CQCC

    ceCEQC cCQCE C C CC

    v RiV R I V vV Ri I v RiV )()(

    (12) 0 cecc v Ri9 2013/2014 EKT204

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    I B versus V BE Characteristic

    b BT

    be BQ B i I V

    v I i )1(

    Time-varying signal source, v s appliedto base - time-varying base currentcomponent

    ==> there is a time-varying base-emitter component

    Figure shows exponential relationship

    between i B vs v BE

    IF MAGNITUDES of time-varyingsignals superimposed on dc Q-pt aresmall => develop linear relationshipbetween ac v BE and ac i B

    This relationship corresponds to slopeof curve at the Q-pt.

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    Rules for AC Analysis

    Replacing all capacitors by short circuits

    Replacing all inductors by open circuits

    Replacing dc voltage sources by ground connections

    Replacing dc current sources by open circuits

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    AC Equivalent Circuitfor Common Emitter

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    EquationsInput loop

    Output loop

    beT

    BQb

    be Bb s

    vV

    I i

    v Riv

    bc

    ceC c

    ii

    v Ri

    00.026 V

    The DC voltage sources have been set equal to zero or ground(V CC =0).Only ACc condition are to be considered.

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    Small Signal AC Equivalent Circuit

    ac input signal voltages and currents are in the orderof 10 percent of Q-point voltages and currents.

    e.g. If dc current is 10 mA, the ac current (peak-to- peak) < 0.1 mA.

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    Small-signal hybrid- equivalent circuit

    BQ F CQ

    CQ

    T F

    BQ

    T

    b

    be

    I I

    I V

    I V

    r iv

    ,

    g m =I CQ /V T

    r = VT/I CQ

    v be = i b r

    r = diffusion

    resistance /base-emitter inputresistance

    1/r = slope of i B

    V BE curve

    14

    Phasor signals are shown in parentheses.

    r g mCommon-Emitter Current Gain, as constant;2013/2014 EKT204

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    )( b

    b

    I

    i

    Using common-emitter current gain ( ) parameter

    Small-signal hybrid- equivalent circuit

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    How to construct Small-signal hybrid-

    Place a terminal for the transistor

    Common Terminal as ground

    B

    E

    C

    We know that

    i across B ib

    i across C i b

    i across E (+1)i b

    r between B -E

    R C

    R B

    v s

    v O

    V BB

    V CC

    B

    E

    C

    ibr

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    C bemceo RV g V V s B

    be V Rr r

    V

    BC m

    s

    ov Rr

    r R g

    V V

    A

    gain,voltagesignalSmall

    Output signal voltage

    Input signal voltage17

    Small-signal Voltage Gain

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    Problem-Solving Technique:BJT AC Analysis

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    1. Analyze circuit with only dc sources to find Qpoint.

    2. Replace each element in circuit with small-signal model, including the hybrid model forthe transistor.

    3. Analyze the small-signal equivalent circuitafter setting dc source components to zero.

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    Transformation of Elements

    Element DC Model AC Model

    Resistor R R

    Capacitor Open C

    Inductor Short L

    Diode +V g, r f r d = V T /I D

    Independent Constant

    Voltage Source

    + V S - Short

    Independent ConstantCurrent Source

    IS Open

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    Example 1

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    Determine the small signalvoltage gain, including theeffect of the transistoroutput resistance, r o.

    Assume the transistor &circuit parameter are =100,VCC=12V, V BE=0.7V,RC=6k, RB=50k andVBB=1.2V.

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    21

    Solution 1Do the dc analysis to find Q-point values

    Determine the small signal output resistance ,

    Do the ac analysis to find the small signal base-emitter input resistance,r , transconductance, g m and then voltage gain, AV

    V k m R I V V

    mA I I

    A RV V

    I

    C CQCC CEQ

    BQCQ

    B

    BE BB BQ

    6)6)(1(12 then,

    1)10(100thatso

    10507.02.1

    k m I

    V r

    CQ

    Ao 50

    1

    50

    4.11506.2

    6.2)6(5.38)(

    /5.38026.0

    1

    6.21

    )026.0(100

    m

    Rr r

    R g V V

    A

    V mAm

    V

    I g

    k m I

    V r

    BC m

    S

    oV

    T

    CQm

    CQ

    T

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    Hybrid- Equivalent Circuitand Early Effect

    transconductanceparameter

    current gainparameter

    r o =V A/I CQ

    r o = small-signaltransistor output

    resistance V A = early voltage22 2013/2014 EKT204

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    Early Voltage(V A )

    Early Effect

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    Example 2 If the Early voltage, V A is 50 V, reconsider thecircuit in example 1 and determine the small-signal voltage gain including the effect of thetransistor output resistance, r 0 .

    24 2013/2014 EKT204

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    Solution 3

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    C omo Rr V g V

    r R R Ri 21 C oo Rr R

    sS

    V Rr R R

    r R RV

    21

    21

    C oS

    m s

    ov Rr Rr R R

    r R R g

    V V

    A

    21

    21

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    Expanded Hybrid- EquivalentCircuit

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    h-Parameter Model for npn

    fe

    bie

    h

    r r r h

    ooe

    re

    r r h

    r

    r h

    11

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    T-Model of an npn BJT

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    4 Equivalent 2-port Networks

    Voltage Amplifier

    Current Amplifier

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    Cont

    Transconductance Amplifier

    Transresistance Amplifier

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    2013/2014 EKT20435

    Small Signal Equivalent Circuit

    If

    The coupling capacitor is assumed to be a shortcircuit. (If signal source >>> 2kHz)

    TH cC R

    fC Z

    2

    1

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    2013/2014 EKT20436

    ExampleDetermine the small voltage gain for the circuit below if=100, VCC=5V, V BE=0.7Vand V A=100V

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    2013/2014 EKT204 37

    SolutionDo the dc analysis to find Q-point values

    V k m R I V V mA I I

    Ak R

    V V I

    V V R R R

    V

    k k

    k k R R

    R R R

    C CQCC CEQ

    BQCQ

    TH

    BE TH BQ

    CC TH

    TH

    31.6)6)(95.0(12 then,95.0)5.9(100thatso

    5.99.5

    7.0756.0

    756.0)12(1003.6

    9.5100

    )3.6)(7.93(

    21

    2

    21

    21

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    2013/2014 EKT20438

    SolutionDetermine the small signal output resistance ,

    Do the ac analysis to find the small signal base-emitter input resistance,r , transconductance, g m and then voltage gain, AV

    k m I V

    r CQ

    Ao 3.10595.0100

    1635.087.1

    87.1)3.105//6(5.36

    ////

    )//(

    /5.36026.095.0

    74.295.0

    )026.0(100

    k m

    R Rr Rr

    r R g V V

    A

    V mAm

    V

    I g

    k m I

    V r

    S TH

    TH oC m

    S

    oV

    T

    CQm

    CQ

    T

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    The basic common-emitter circuit used inprevious analysis causes a serious defect :

    If BJT with V BE =0.7 V is used, I B=9.5 A & I C=0.95 mA

    But, if new BJT with V BE =0.6 V is used, I B=26 A & BJTgoes into saturation; which is not acceptable Previouscircuit is not practicalSo, the emitter resistor is included: Q-point is stabilizedagainst variations in , as will the voltage gain, A V

    AssumptionsCC acts as a short circuitEarly voltage = ==> r o neglected due to open circuit

    Basic Common-Emitter Amplifier

    39

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    2013/2014 EKT20440

    Circuit with Emitter ResistorTo improve dc biasing designAV with R E less dependent on.VA infinite, r o open circuit.

    C bo R I V )(tage,output volac

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    Common-Emitter Amplifierwith Emitter Resistor

    ac output voltage

    Input voltage loop

    Input resistance, R ib

    Input resistance to amplifier, Ri

    Voltage divider equation of V in to V s

    Remember : Assume VA is infinite , r o is neglected

    C bo R I V

    E bbbin R I I r I V

    E b

    inib Rr I

    V R 1

    ibi R R R R 21

    s

    S i

    iin V

    R R

    RV

    41

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    2013/2014 EKT20442

    E

    C

    E

    C V

    E si

    si

    i

    E

    C

    ib

    in

    s

    C

    s

    C b

    s

    oV

    s si

    iin

    ibi

    E

    b

    inib

    E bbbin

    R R

    R R

    A

    r R R R

    R R R

    Rr R

    RV

    V R

    V R I

    V V

    A

    V R R

    RV

    R R R R

    Rr I

    V R

    R I I r I V

    )1(

    )1( and if

    )1()(

    ////,resistanceinput

    effectrulereflectionresistance)1(

    )(

    21

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    2013/2014 EKT20443

    Example

    Determine the small voltage gain for the circuitwith an emitter resistor below if =100,VBE=0.7Vand V A=.

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    2013/2014 EKT20444

    Solution

    0.5

    )1( and if

    53.4

    06.8////

    6.41)1(

    /1.83

    2.1

    81.4;16.2

    21

    V

    E si

    s

    oV

    ibi

    E b

    inib

    CQ

    A

    o

    T

    CQm

    CQ

    T

    CEQCQ

    A

    r R R R

    V V A

    k R R R R

    k Rr I V

    R

    I V

    r

    V mAV

    I g

    k I V

    r

    V V mA I

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    2013/2014 EKT20445

    Circuit with Emitter BypassCapacitor

    Use to effectively to short out a portion @ all of emitterresistance by the ac signal .

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    R S

    R 1

    R 2 R E

    R C

    vs

    vO

    C C

    V CC

    C E

    B C

    E

    V o

    V s R C

    RS

    r r oR 1||R 2

    g m V

    Emitter bypass capacitor, C E provides a s h o r t c i r c u i t toground for the ac signals

    Common-Emitter Amplifierwith Emitter Bypass Capacitor

    Small-signal hybrid-

    equivalent circuit

    Emitter bypass capacitor isused to short out a portion orall of emitter resistance bythe ac signal. Hence no REappear in the hybrid- equivalent circuit

    46

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    Common-emitter Amplifier withEmitter Bypass Capacitor

    47

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    AC Load Line - KVL on C-E loop

    1

    11

    1

    1- Slope

    )(

    Assuming

    0

    E C

    E C c E cC cce

    ec

    E eceC c

    R R

    R Ri Ri Riv

    ii

    Riv Ri

    49

    Visualized the relationshipbetween small-signalresponse & transistorcharacteristics

    Occurs when capacitorsadded in transistor circuit

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    50

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    Example (DC & AC Load Line)

    Determine the dc and ac load line. V BE=0.7V, =150, VA=

    51

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    Solution

    To determine dc Q-point, KVL around B-E loop

    k R R-

    R I R I V V V

    mA I I mA I I

    A R R

    V V I

    R I V R I R I V R I V

    E C

    E EQC CQCEQ

    BQ EQ BQCQ

    E B

    EB BQ

    E BQ EB B BQ E E EB B BQ

    1511 Slope

    53.6)( point,-QFor

    9.0)1( & 894.0Then

    96.5)1(

    )1(

    52

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    )//()//)((

    /4.34

    36.4

    53.6;894.0

    LC c LC meo

    CQ

    Ao

    T

    CQm

    CQ

    T

    ECQCQ

    R Ri R Rv g vv

    I V

    r

    V mAV

    I g

    k I

    V r

    V V mA I

    53

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    Maximum Symmetrical Swing

    When symmetrical sinusoidal signal applied to theinput of an amplifier, the output generated is alsoa symmetrical sinusoidal signal

    AC load line is used to determine maximumoutput symmetrical swing

    If output is out of limit, portion of the output signal willbe clipped & signal distortion will occur

    55

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    Maximum Symmetrical Swing

    Steps to design a BJT amplifierWrite DC load line equation (relates of I CQ & V CEQ)Write AC load line equation (relates ic , vce ; vce = - icReq ,Req = effective ac resistance in C-E circuit)Generally, ic = I CQ I C (min), where I C (min) = 0 or someother specified min collector currentGenerally, vce = V CEQ V CE(min), where V CE(min) issome specified min C-E voltageCombination of the above equations produce optimumI CQ & V CEQ values to obtain maximum symmetricalswing in output signal

    56

    E l (M i S i l S i )

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    Example (Maximum Symmetrical Swing )

    Determine the maximum output symmetrical swing for the ac loadline in previous figure.

    SolutionFrom the dc & ac load line, the maximum negative swing in the I c is from0.894 mA to zero (I CQ). So, the maximum possible peak-to-peak ac

    collector current:

    The max. symmetrical peak-to-peak output voltage:

    Maximum instantaneous collector current:

    mA79.1)894.0(2(min))(2 C CQc I I i

    V56.2)2||5)(79.1()||(|||||| LC ceqcce R Ri Riv

    mA79.1894.0894.0||21

    cCQC i I i

    57

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    C-C Small Signal Voltage Gain

    CommonCollector Circuit

    Small SignalEquivalent

    Circuit

    58

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    )//(

    )1(

    E ooo

    bo

    Rr I V

    I I

    si

    i

    E o

    E o

    s si

    iin

    E oib

    ibb E obobin

    R R R

    Rr r Rr

    V R R

    RV

    Rr r R R I Rr r I V r I V

    )//)(1()//)(1(

    VV

    A

    gainvoltagesignalSmall

    )]//)(1([

    )]//)(1([

    s

    ov

    59

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    C-C Input & Output Impedance

    x

    xo I

    V R

    o E s

    o

    oo E s x

    x

    m

    s

    x

    o

    x

    E

    x x

    s

    m x

    s

    x

    o

    x

    E

    xm x

    x s

    s

    x

    o

    x

    E

    xm x

    r R R R Rr

    R

    Rr R R R Rr V I

    r g

    R R Rr V

    r V

    RV

    V R R Rr

    r g I

    R R Rr V

    r V

    RV

    V g I

    V R R Rr

    r V

    R R Rr V

    r V

    RV

    V g I

    ////1

    //// therefore,

    111////

    1

    that Note

    ////////

    //// therefore,

    ////

    ////

    nodeoutputatcurrentsSumming

    21

    21

    2121

    21

    21

    21

    60

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    ExampleCalculate

    the small signal voltage gain,the input and output resistance.

    Assume the transistor & circuit parameter are; =100, VCC=5V,VBE=0.7V, V A=80V and r o=100k.

    61

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    C-C Small Signal Current GainCan be determine by using the input resistance & the concept ofcurrent dividers.

    )1(

    then,R r andR //R R thatassumeIf

    ////

    )1(

    Therefore,

    ////)1()1(

    ////

    Eoib21

    21

    21

    21

    21

    21

    21

    i

    E o

    o

    ibi

    ei

    o E o

    oe

    iib

    bo

    iib

    b

    i

    ei

    A

    Rr r

    R R R R R

    I I

    A

    I Rr

    r I

    I R R R

    R R I I

    I R R R

    R R I

    I I A

    62

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    Common Base Amplifier

    63

    C B S ll Sig l E i l t

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    C-B Small Signal EquivalentCircuit

    64

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    C-B Small Signal Voltage Gain

    zero]approachesR [as )//(

    ////11

    )//(

    ////1

    then,

    since 111

    E]nodeatEquation[KCL 0)(

    )//)((

    S LC mV

    S E S

    LC m s

    o

    V

    S E S

    s

    mS

    s

    S E

    S

    s

    E m

    LC mo

    R R g A

    R Rr

    R R R g V V

    A

    R Rr

    RV

    V

    r g R

    V

    R Rr V

    RV V

    RV

    r V

    V g R RV g V

    65

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    C-B Small Signal Current Gain

    infinity]approachesREandzeroapproachesR [as 1

    1

    //1

    then,

    )(

    //1

    E]nodeatEquation[KCL 0

    L

    r g A

    Rr

    R R R

    g I I

    A

    R R RV g I

    Rr

    I V

    RV

    r V V g I

    mi

    E LC

    C m

    i

    oi

    LC

    C mo

    E i

    E mi

    66

    d

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    Input Impedance

    ei

    ie

    mmbi

    r r

    I V

    R

    r V V g

    r V

    V g I I

    1

    resistanceInput

    1

    inputat theKCL

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    Output Impedance

    C o

    S E m

    R R

    RV

    RV

    r V

    V g

    resistanceoutputThe

    0Vgmeans0,VimpliesThis

    0

    emitter at theKCL

    zero.toequalset beenhasv

    m

    s

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    Summary & ComparisonConfiguration Common

    EmitterCommonCollector

    Common Base

    Voltage Gain Av > 1 Av 1 Av > 1

    Current Gain Ai > 1 Ai > 1 Ai 1

    InputResistance

    Moderate(k)

    High(50-100k)

    Low()

    OutputResistance

    Moderate toHigh

    Low Moderate toHigh