Multipliers Applications

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    IC MultipliersApplicatrions

    Recommended Text: Sergio Franco, Design with

    Operational Amplifiers and Analog Integrated

    Circuits. McGraw-Hill, (1988) pp. 538-548

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    Introduction

    Nonlinear operations on continuous-valued analogsignals are often required in instrumentation,

    communication, and control-system design. These operations include

    rectification,

    modulation - demodulation, frequency translation,

    multiplication - division.

    non-linear function In this chapter we analyze the most commonly used

    techniques for performing this within a monolithic

    integrated circuit

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    In analog-signal processing the need often arises for a circuit

    that takes two analog inputs and produces an output proportional

    to their product. Such circuits are termed analog multipliers.

    There are two different approaches to analog multipliers

    One of them is based on log/antilog amplifiers Another utilizes the exponential transfer function of bipolar

    transistors (Gilbert cell) .

    In following sections we consider applications of IC multipliersbased on both approaches

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    Log/Antilog Converter

    The log and antilog functions can be combined in slide rule

    fashion to perform such operations as

    multiplication, division,

    exponentiation, and

    root computation.

    Two of the most useful functions are

    multifunction conversion and

    true rms-to-dc conversion

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    Multifunction Converters

    A multifunction converter (4302) is a circuit that accepts three inputs, Vx, Vy,

    and Vz and yields an output Vo of the type: m

    x

    zyo

    V

    VKVV

    =

    where Kis a suitable scale factor (typically K = 1),

    and m is a user-programmable exponent, in therange 0.2 < m < 5

    where K is a suitable scalefactor (typically K = 1),

    and m is a user-programmable exponent, inthe range 0.2 < m < 5

    By proper selection of

    input configuration andexponent, the circuit can beprogrammed for a varietyof operations:

    etc./1,,,/, xn

    z

    m

    zzxyxo VVVVVVVV =

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    With the help of simple op amp circuitry it can be configured

    for additional operations, such as

    non-integer exponent approximations, coordinate conversion, and

    true rms-to-dc conversion.

    Although now the tendency is to implement these functions

    digitally, considerations of cost and speed often require their

    implementation in analog hardware.

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    4302 block diagram

    The circuit diagram of 4302 is shown with frequency compensation and

    reverse-polarity protection omitted for simplicity.

    By op amp action, we have

    x

    x

    x R

    VI =

    y

    y

    y R

    VI =

    z

    zz

    R

    VI =

    o

    oo

    R

    VI =

    The voltages at pins 6

    and 12 are proportional

    to the log ratios of thecorresponding currents:

    =

    x

    zTI

    IVV ln6

    =

    y

    o

    T I

    IVV ln

    12

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    m=1

    V6

    and V12

    are derived directly from V11

    so that V6

    = V12

    = V11

    .

    By this impliesIz/I

    x= I

    o/I

    ythat is,

    Vz/V

    x= V

    o/V

    y.

    Thus,

    ( ) yoTxzT IIVVIIVV /ln/ln 126 ===

    =

    x

    z

    yo V

    VVV

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    m1

    m < 1: V6

    is derived directly from V11

    while V12

    is derived from V11

    via a

    voltage divider, V12

    =mV11

    , where m=R2/(R1+R2).

    Letting V12

    =mV6

    yields ,

    that is,

    This, in turn, yields ,

    that is,

    3. m > 1: V12 is derived directly from V11 while V6 is derived from V11 via avoltage divider, V6=(1/m)V

    11, where (1/m)=R2/(R1+R2).

    Letting V6=V

    12/m yields

    m

    xzxzyo IIIImII )/ln()/ln()/ln( ==m

    xzyo IIII )/()/( =m

    xzyo VVVV )/()/( =

    121

    2where, +=

    =

    RRRm

    VVVV

    m

    x

    zyo

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    Multiplication and Division

    E ti t d

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    Exponentiator andRoot Extractor

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    4302 Adjustment

    In each con-figuration the scale factor is calibrated by setting the input(s) to

    10 V and adjustingRy for Vo = 10 V.

    To maintain the accuracy of division at low signal levels, the input offset

    errors of the X and Z op amps must be nulled as follows

    1. With Vz = Vx = 10.0 V, adjust R1 for Vo = 10.0 V.

    2. With Vz = Vx = 100 mV, adjustR2 for Vo = 10.0 V.

    3. With Vx = 100 mV and Vz = 10.0 mV, adjust R3 for Vo = 1.00 V. Repeat the procedure, if necessary.

    The 4302 provides the following typical accuracies expressed as a percent of

    the output full scale:

    multiply, 0.25 percent;

    divide, 0.25 percent;

    square, 0.03 percent;

    square root, 0.07 percent.

    F d t lti li

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    Four-quadrant multiplierAD534

    Figure shows the complete multiplier AD534.

    Four-quadrant operation is achieved by using two transconductance pairs

    with the bases driven in antiphase and the emitters driven by a second V-I

    converter. ))(( 212121 YYXXKZZ =

    xxy

    z

    IRR

    RK =

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    AD534 Basic Configuration

    The basic connection for four-quadrant multiplication, is used in

    amplitude modulation,

    voltage-controlled amplification, and

    instantaneous power measurements.

    When one of the inputs is zero,

    the output should also be zero,

    regardless of the signal at the other input. In practice, a small fraction of the other input will feed through to the output,

    causing an error.

    This can be minimized by applying an external voltage to theX2 or Y2 input.

    This basic configuration has a number of useful variations.

    For instance, tying the inputs together yields the squaring function.

    Deriving Z1 from Vo via a voltage divider allows for scale factors other than

    1/(10 V). Applying a signal to theZ1 terminal will cause it to be summed to the output

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    AD534 Applications

    ))(( 212121 YYXXKZZ =

    )()10/1( oxz VVV =

    ozo VVV /10=

    )()10/1( ooz VVV =

    zo VV = 10

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    Show that ( ) 10/22 yxo VVV =