Current Sources Slide

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    A simple two-transistor current source.

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    Ic1 = Ic2

    Summing currents at the collector of Q1

    yields

    021

    1!

    F

    Ccref

    III

    Fand thus

    212

    1

    C

    F

    ref

    C I

    I

    I !

    !

    F

    ifFF is large, the collector current of Q2 is nearly equal to the

    reference current:

    R

    VVII

    onBECC

    refC

    )(

    2

    !$

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    Simple current source with current gain.

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    The emitter current of transistor Q3 is equal to

    2

    21

    3

    2

    C

    FF

    C

    F

    CE I

    III

    FFF!!

    The base current of transistor Q3 is equal to

    2

    3

    3

    1

    2

    1C

    FFF

    EB I

    II

    !

    !

    FFFFinally, summing currents at the collector of Q1, we obtain

    0

    1

    221

    !

    CFF

    Cref IIIFF

    Since IC1 and IC2 are equal,

    FF

    ref

    Co

    III

    FF

    !!

    2

    22

    1

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    Widlar current source

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    Summing voltages around the emitter-base loop, assuming that

    VA is infinite, and neglecting base currents results in

    022

    2

    2

    1

    1 ! RI

    I

    IInV

    I

    IInV C

    S

    CT

    S

    CT

    For identical transistors, IS1 and IS2 are equal, the equation

    becomes

    22

    2

    1RI

    IIInV CS

    CT !

    02221 ! RIVV CBEBE

    and thus

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    Cascode current source with bipolar transistors.

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    Thus, cascode current sources can boost the output resistance

    and equivalent open-circuit voltage approximatelyF0 / 2.

    ForF0 = 100 and VA =130V, we have

    VVIr

    V AooThev 650022

    00 !!!FF

    At an output current Io = 1mA, we find that

    ;!! M

    mA

    VRo 5.6

    1

    6500

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    N-Channel mirror

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    In the most general case, the ration of iO to iI is

    -

    !

    1

    2

    1

    2

    2

    1

    2

    21

    21

    1

    1

    K

    K

    vv

    VV

    VV

    LW

    WL

    i

    i

    DS

    DS

    TGS

    TGS

    I

    O

    PP

    -

    !1

    2

    21

    21

    1

    1

    DS

    DS

    I

    O

    v

    v

    LW

    WL

    i

    i

    P

    P

    If vDS2 = vGS1, then the ratio of iO/iIbecomes

    !

    21

    21

    LWWL

    ii

    I

    O

    -

    !

    1

    2

    11

    DS

    DS

    I

    O

    vv

    ii

    PP

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    The Differential Amplifier

    The emitter-coupled or differential pair stage

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    CmCo

    DM

    oDM Rg

    r

    R

    V

    VA !!!

    T

    F1

    Small-signal models for(a) the differential mode and (b) the common mode.

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    Common-Mode Gain ACM

    TFF

    rR

    R

    V

    V

    A Eo

    Co

    CM

    o

    CM

    !! 12

    1

    with Fo >> 1 and division by rT, reduces to

    E

    C

    Em

    CmCM

    R

    R

    Rg

    RgA

    221

    }

    !

    The 2gmRE >> 1. Because the same signal is applied to Q1 and Q2,

    both Vo1 and Vo2 are 180o out of phase with VCM.

    The Common-Mode Rejection Ratio:

    CM

    DM

    A

    ACMRR !

    CMRR = 1 + 2gmRE } 2gmRE

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    Output for Arbitrary Input signals

    22

    21 d

    DM

    VVV

    V !

    ! 2

    21VV

    VCM

    !

    The output voltage Vo1 is

    CMCMDMDMO VAVAV !1

    !CMRR

    VVA CMDMDM

    ! CMRR

    VVV

    AV d

    DMo

    21

    1

    2

    !

    CMRR

    VVV

    AV

    d

    DMo

    21

    22

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    A source-coupled pair

    For rd >> RD and Q >>1,

    SgmSgm RRCMRR 221 }!

    FETDifferential Amplifier

    Dd

    S

    Rr

    RCMRR

    !

    Q121