M&I Notes-10

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    University of Engineering and Technology Taxila

    Mechanical Engineering Department

    Lecture No: 10

    Course Title: Measurement and

    Instrumentation (ME-!"#

     Tutor: $halid Masood $han

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    Measurement of &orce

    •  &orce tends to change state of a'ody 'eing

      either at rest or in motion

    •  uantitatively) force is e*ual to

    the rate of   change of momentum of the 'ody •  &orce is de+ned from thefundamental

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    ,oad Cells•  The term is used to descri'e atransducer that  generates a signal as a result of anapplied  force) usually along a particular

    direction

    •  These transducers often consist of an

      elastic mem'er and a deection

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    •  These deection sensors mayemploy

      changes in capacitance)resistance) or the  pie.oelectric e/ect to sense

    deection

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    Categories of ,oad Cells•   1train 2auge ,oad Cells

    •   3roving 4ing

    •   3ie.oelectric ,oad Cells

    ,oad cells may 'e characteri.ed as 'eam-type

    load cells) proving) or columnar-type

    designs

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    1train 2auge ,oad Cells

    •  These are designed 'y using alinearly  elastic mem'er instrumented 7ithstrain  gauges

    •  The shape of the linearly elasticmem'er  should meet the follo7ing

    re*uirements

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    •  It should provide an appropriaterange of   force measuring capa'ility 7ithnecessary

      accuracy

    •  It should provide sensitivity to forces

    in a  particular direction

    •  It should have lo7 sensitivity toforce

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     Types of 1train 2auge ,oad Cell

    •   ending eam ,oad Cell

    •   1hear eam ,oad Cell

      ;ithin the elastic range) the 'ending  stresses are linearly related to applied loads

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    ending eam ,oad Cell

    •  The sensing element functions as a

      cantilever 'eam

    •  1train gauges are mounted on the

    top and  the 'ottom of the 'eam tomeasure normal

      or 'ending stresses

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    !!

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    1hear eam ,oad Cell

    •  The 'eam cross-section is that of anI-'eam

     •  1hear stress in the 7e' is constant

      In general) 'ending 'eam load cellsare less  costly 'ecause of their construction=>o7ever)  shear 'eam load cells have several

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    3roving 4ing

    •  ? ring type load cell can 'e employedas a local

      force standard

    •  1uch a ring-type load cell is oftenemployed in

      the cali'ration of materials testingmachines  'ecause of the high degree of

    precision and

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    •  If the sensor is approximated as a

    circular  right cylinder) the relationship'et7een

      applied force and deection isgiven 'y

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    •  The application of proving ring

    involves  measuring the deection of theproving

      ring in the direction of theapplied force

      Typical methods for thisdisplacement  measurement includedisplacement  transducers) 7hich measure

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    3ie.oelectric ,oad Cells

    •  3ie.oelectric materials arecharacteri.ed 'y

      their a'ility to develop a charge7hen su'@ect  to a mechanical strain

    •  The most common pie.oelectricmaterial is a

      single crystal *uart.

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    •  The modulus of elasticity of

    *uart. is  approximately 80 23a) yielding

    load cells  7ith typical static sensitivitiesranging  from

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    1ection-B%8th ovem'er %

    ?ssignment:Measurement of ow velocity

    0th Dec %

    UI T?$E(%#(3ie.oelectric load cell designFDra7 simple +gure and identifydi/erent components #

    ?11I2MET CG,,ECTED