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02 Position c 0

Date post: 03-Apr-2018
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    Inductosyn Position-dependent mutual inductance (and thus signal

    transfer) between two meander-like flat coils

    Excitation:

    current into the fixed scale, OR

    current into the moving slider

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    Inductosyn driven slider

    * One rotor (slide) driven by current

    tKUtutU == coscos)(cos 2

    * Two rotors driven

    )cos()cossincos(cos)(u)(u)(u 22212 =+=+= tKUttKUttt

    == cos)2cos(2 KUpxKUU

    Coarse scale: incremental, fine scale : measurement of phase

    Mutual inductance

    M ~cos

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    Inductosyn - driven stator (scale)

    sincos)(usinsin)(u 2221 tKUttKUt ==

    tKUtKUtu == sin)sin(sin)sincoscos(sin)(3

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    stator

    rotor

    stator

    rotor

    a) b)

    Resolver Selsyn

    Scott transformer (3 phase / 2 phase)

    Conversion of selsyn signal to resolver form

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    Sensors based on eddy currents

    the depth of field penetration (attenuation to 1/e)

    G

    Zm

    y

    i~

    a) b)

    2

    =

    Difficult field penetration to conductors

    (low resistivity => high eddy currents)

    Used for detecting presence of conductive targets

    (proximity switch)

    !!!

    Eddy currents in

    the material

    compensate the

    external field

    (Lenz law)

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    Sensors based on eddy currents -construction

    field concentration (focusing) :ferrite core, ev. magnetic shielding

    The sensor in typical

    threaded-cylinder shape

    Metallic target

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    Sensors based on eddy currents :

    signal conditioning circuits

    Bridge and transformer circuits (compensating sensor) resonant circuits LC-oscillator: f, Q

    pulse driven - defectoscopy

    low f: change of Re(Z)

    high f: change of L

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    Sensors based on eddy currents : applications

    sensors of translational motion

    binary sensors of position (proximity switch)

    detection of vehicles (or any conducting objects - mines, cable,pipelines)

    diagnostics

    cracks

    material composition

    noncontacting

    operation in presence of dirtiness

    target conductive

    for d > independent on target parameters

    u2

    um

    u1

    us

    is

    iw

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    ~

    ~

    1

    2

    e)

    ~

    d)

    ~ 1

    2

    b)

    ~

    k)

    ~

    h)

    ~

    a)

    ~

    g)

    ~

    j)

    ~

    l

    c)

    ~

    f)

    ~

    i)

    l

    ~

    l)

    Sensors based on eddy currents : applications

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    Magnetostictive sensors of position

    max. length up to 4 m (attenuation)

    hysteresis 0.4 m linearity 0.02 %

    elastic wave in ferromagnetic material .... v = 3000 m/s = 3m / ns (approx. 10x speed of sound in air)

    Interaction of magnetic fields (current pulse + permanent magnet) creates pulse of mechanical strain

    (Wiedemann effect ) propagating along the wire. Time of flight => position of permanent magnet

    S N S N S NSN SN SN

    Inductionpickup coil

    Magnetostrictivewire

    Magnet inmovablefloat

    InnerTube

    Outerguide tube Reflectionterminator

    Strain pulse

    Strain pulse Strainpulse

    reflectedoff bottom

    Inductionpickupsensesinitial andreflectedstrainpulses

    A B C

    Patriot

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    Capacitive sensorsd

    SC

    =

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    Capacitive sensors contdd

    SC

    =

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    Capacitive sensor with variable

    area of electrodes overlapping

    -

    1323

    1323

    CC

    CC

    +

    dSC =

    a)

    b)

    13

    2

    x

    +xx

    C C13 23+C13

    C23

    ratiometric measurement: influence ofd, eliminated

    C i i i h i bl

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    Capacitive sensor with variable

    area of electrodes overlapping

    2313

    2313

    V23213

    21

    232131

    232131232131

    u)()(

    U,if

    )()()(U)(U0)(U)(U

    CC

    CC

    UCUuCUu

    UUU

    CUuCUuCjCjCjjCjj

    VV

    VV

    +

    =+=

    ==

    ===+

    resolution: 1 m, uncertainty 5 m

    a)

    b)

    13

    2

    x

    x

    x

    x

    +xx

    C C13 23+C13

    C13

    C23

    C23

    1

    2

    u1

    u ; u1 2

    U1

    U1

    U1

    u2

    U2U2

    U2

    u3uv

    uv

    uv

    3

    P1

    P2

    Reg.

    c)

    td)

    1 2

    3

    3

    1 2

    e)

    f)

    S

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    Modern signal conditioning circuits for

    capacitive sensors

    Main problem -

    influence of capacitance of leads (cable)

    (driven from voltage source, current measured by ideal

    ammeter )

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    charge pump

    realisation by CMOS technology and inductive dividers

    coils and transformers are not necessary

    C/f converter

    ADC not necessary

    converter C/U capacitor in feedback eliminates dependence on frequency

    transformer bridges

    expensive, noncompatible with IC

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    +

    Cp2

    C1

    Cp1 Cs

    G

    U (j )1

    U (j )2 U(j )

    -A

    Linearity even for variable air gap sensor (vibration measurement),U2 ~ d

    Amplifier for capacitive sensors:

    Parasitic capacitances of the cable to Cs will not apply:

    Cp1 is on virtual zero, Cp2 is on low output impedance of the OpAmp

    Applications of capacitive sensors

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    Applications of capacitive sensors

    Honeywell

    Omeg

    Sensing humidity of

    material in dryer

    Sensing level of liquid dye in

    printworks

    Bottle

    Conveyor

    belt

    Control of filling

    drums

    reservoir

    Checking presence of parts

    in product completionControl of filling

    Typical applications:- sensing level in tanks

    - checking filling of products

    inside packages- sensing level of powder /

    granules in storage

    - sensing non-metalic objects

    on conveyor belts

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    Hone well

    rubber gasket

    sensor

    Checking presence of products in mass production:

    sensor

    metal object


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