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    Innovative -I

    In Experimental Methods

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    1.Introduction

    2.Types

    3.Peizo resistive type

    4.Peizo electric type

    5.Summary

    6.Reference

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    A semi-conductor may be defined as an electrical

    conductor that has a conductivity intermediate

    between that of an insulator and that of a

    conductor.

    The conductivity of semiconductor materials can

    be changed radically by small changes in physical

    condition.

    Semi conductors are prepared by diffusing

    impurities to pure silicon or germanium crystals.

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    Very high conductor sensitivities are possible

    Negative gauge factors are possible in semi-

    conductor gauges which permits large

    electrical output from Wheatstone bridegecircuit.

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    The semi-conductor gauges are of two types

    1. PEIZO RESISTIVE GAUGES

    2. PEIZO ELECTRIC GAUGES

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    Peizo resistive effect is the phenomenon inwhich the change in resistance of a semiconducting material accompaniesdeformation.

    It was first demonstrated by Mr.Smith in 1954

    on Silicon and Germenium.

    This type of strain gauges are useful forstatic strain measurments.

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    They are produced from single crystal silicon

    or germanium.

    Boron is used as trace impurity for producing

    p-type conductor. Arsenic is used to produce the N-type

    The resistivity od p-type silicon is in the

    order of 500 .

    This very high sensitivity is reason why theyare used in measuring extremely small

    strains .eg.in tranducers

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    Semi conductor filaments of even smaller

    cross sections can be constructed by

    condensation of silicon vapour on the cool

    walls of a quartz tube.

    The lead material for the semi-conductor

    filament is generally doped with a small

    amount of antimony. P-type gauges are used in tensile fields and

    N-type gauges are used in compressive fields.

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    Semi conductor strain gauges can be classified

    with respect to following characteristics.

    Filament material (p or n type)

    Gauge factor Gauge length

    Gauge resistance

    Temp compensation

    Backing

    Bonding techniques.

    Lead Geometry.

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    Sensitivity

    The strain sensitivity or gauge factor ,

    F=( R/R) /( L/L)

    = 1+2v+m

    Where m= ( p/p)/( L/L)

    v= poissons ratio

    The factor m accounts for piezoresistiveeffect and (1+2v ) is dimensional effect.

    Usually its value ranges from 50-175.

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    Linearity

    They depend strongly on strain levels and

    are distinctly non-linear.Increase amount of

    impurity may improve the linearity.Temperature Effect

    Environmental temperature changes affect

    the resistance and the sensitivity of

    semiconductor which depends on the levelof doping.

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    Current carrying Capacity

    The maximum permissible current for a

    bonded semi conductor strain gauge depends

    upon the mechanism of heat dissipation,

    mainly conduction to test structure.

    Breaking StrengthIt depends mainly on filament cross section

    For filament cut from from Gauge crystals

    ,the breaking strength is 3x10 3 N/m2

    Hysteresis and creepSemi conductor filament is not responsible

    for any hysteresis or creep errors

    experienced in practical gauge installation.

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    Fatigue

    Fatigue life of semi-conductor gauge ishigher than that of wire and foil gauge.

    Humidity

    semi-conductor gauges are not that much

    affected by moisture.

    Temperature compensation

    Temperature compensation of semi-

    conductor gauges can be achieved in twoways

    1. self compensation

    2. Circuit compensation

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    Introduction

    Certain crystals when mechanically strained

    in particular directions will becomeelectrically polarised.

    The change can be measured by applying

    electrodes to the surfaces and measuring the

    potential difference between them. Substances which possess this property are

    called peizoelectric.

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    In single piezoelectric plates,five operation

    modes are there1. Thickness expansion mode

    2. Length expansion mode

    3. volume expansion mode

    4. Thickness shear mode

    5. Face shear Mode

    For strain gauge applications we use

    Length-expander mode of operations. Peizoelectric crystals can be stacked and it

    can be connected in parallel(higher output)

    or in series(lower output).

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    The peizoelectric materilas are of two type

    A. Naturally occuring type .

    B. Synthetic Materialls.

    Eg: A type1.Quartz(SiO2)

    2.Rochelle salt(NaKC4 O6.4H2o)

    B type1.Barium titanate(Ba Ti O3)

    2.Lead zirconate titanate

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    If a thin slab of peizoelectric material is

    cemented to a structure under stress, the

    strain in the structure is transmitted to the

    slab and a charge is generated across the

    crystal.

    Out put voltage ,V=ht

    h= h-coefficient

    =absolute dielectric constantt=thickness of crystal

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    The crystals are cheap

    Light weight

    Highly sensitive to small stains

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    The high sensitivity of semi-conductor gauges

    make them very useful in steam turbine

    blades.

    Semi-conductor strain gauges of permits thedesign of wide range of subminiature

    transducers which have high natural

    frequency and high output signal.

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    JAMES.W.DALLY AND WILLIAM F.RILEY

    Experimental stress analysis, Mc GRAW-HILL

    BOOK Company , second edition 1987,

    pp 204-215.

    Dr. Sadhu singh , Experimental Stress Analysis ,

    Khanna Publishers,4th edition 2004,

    pp 245-280.

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    Thank You