Mechatronics_Session 3_ Position Sensors

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    MECHATRONICS

    Unit 1

    Classification of Sensors & Transducers(Session-5

    Mec!anical En"ineerin" #e$art%ent

    ' Uniersit)

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    'earnin" O*+ecties

      In t!is lecture students ,ill learn•  Classification of sensors•  Classification of transducers

    •  #is$lace%ent transducers•  Resistance transducers•  Ca$acitie transducers•  Inductance *ased transducers

    •  O$tical encoders 

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    Classification of Sensors

    1. Actie and .assie sensors

    /0 Contact and non-contact sensors0 A*solute and relatie sensors

    20 Ot!er sc!e%es

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    10 Actie and $assie sensors

    .assie Sensor  a sensor t!at re3uires e4ternal $o,er too$erate0

    E4a%$les t!e car*on %icro$!one t!er%istors strain"au"es ca$acitie and inductie sensors etc0

    Ot!er na%e $ara%etric sensors (out$ut is a function of a $ara%eter - li6e resistance

    Actie Sensor  "enerates its o,n electric si"nal and does

    not re3uire a $o,er source0E4a%$les t!er%ocou$les %a"netic %icro$!ones $ie7oelectric sensors0

      Ot!er na%e self-"eneratin" sensors

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    /0 Contact and noncontact sensors

    Contact sensor  a sensor t!at re3uires $!)sical

    contact ,it! t!e sti%ulus0

    E4a%$les strain "au"es %ost te%$erature sensors

     Non-contact sensor re3uires no $!)sical contact0E4a%$les %ost o$tical and %a"netic sensors

    infrared t!er%o%eters etc0

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    0 A*solute and relatie sensors

    A*solute sensor  a sensor t!at reacts to a sti%ulus on

    an a*solute scale

    E4a%$les T!er%istors strain "au"es etc0

    (t!er%istor ,ill al,a)s read t!e a*solute te%$erature

    Relatie sensor  T!e sti%ulus is sensed relatie to a

    fi4ed or aria*le reference0

    E4a%$les T!er%ocou$le %easures t!e te%$erature

    difference $ressure is often %easured relatie to

    at%os$!eric $ressure0

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    20 Ot!er sc!e%es

    Classification *) *road area of detection10Electric sensors

    /0Ma"netic

    0Electro%a"netic

    20Acoustic50C!e%ical

    80O$tical

    90Heat Te%$erature

    :0Mec!anical

    ;0Radiation

    1

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    20 Ot!er sc!e%es (cont0

    Classification *) $!)sical la,

    10.!otoelectric/0Ma"neto electric

    0T!er%oelectric

    20.!otoconductie

    50Ma"nitostrictie80Electrostrictie

    90.!oto%a"netic

    :0T!er%oelastic

    ;0T!er%o%a"netic1

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    20 Ot!er sc!e%es (cont0Classification *) s$ecifications

    10Accurac)

    /0Sensitiit)0Sta*ilit)

    20Res$onse ti%e

    50H)steresis

    80>re3uenc) res$onse90In$ut (sti%ulus ran"e

    :0Resolution

    ;0'inearit)

    1

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    20 Ot!er sc!e%es (cont0Classification *) area of a$$lication

    10Consu%er $roducts 1/0 Scientific

    /0Militar) a$$lications

    0Infrastructure

    20Ener")

    50Heat

    80Manufacturin"

    90Trans$ortation

    :0Auto%otie

    ;0Aionic

    1

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     Classification of transducers10 =ased on $rinci$le of transduction

      (a T!er%o electric

      (* Ma"neto resistie

      (c Electro 6inetic

      (d O$tical

    /0 Actie & $assie

    0 Analo" & di"ital20 Inerse transducer 

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     .assie transducer #eice ,!ic! derie $o,er re3uired for

    transduction fro% au4iliar) $o,er source - e4ternall) $o,ered

    E4a%$le  resistie inductie ca$acitie

    ?it!out $o,er t!e) ,ill not ,or6   Actie transducer 

      No e4tra $o,er re3uired to $roduce I@$

      Self "eneratin"  #ra, $o,er fro% in$ut a$$lied

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    Analo" transducer  conert I@$ 3uantit) into an analo" o@$

    Analo" o@$- a continuous fn0 Of ti%eE"0 Strain "au"e ' #T t!er%ocou$le

      #i"ital transducer 

    Conerts I@$ into an electrical O@$ in t!e for% of $ulses

    Inerse transducer 

    ?!ic! conerts electrical si"nal to $!)sical 3uantit)

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    Inductie Transducers

    T!ere is a ariet) of transducers ,!ose o$eration isinductie0

    B >or %otion %easure%ent a$$lications a c!an"e in t!e

    3uantit) to *e %easured %ust *e conerted into a c!an"e in

    inductance (and t!en to olta"e usin" a circuit0

    • ?e first reie, inductanceDD *riefl)0

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    Inductance

    • A %a"netic field can *e isuali7ed *) lines of %a"netic

    force0 T!e entire "rou$ of %a"netic field lines is called

    %a"netic flu40

    B Ma"netic field lines are $racticall) unaffected *)

    non%a"netic %aterial suc! as air acuu% $a$er "lass,ood and $lastics0 Ho,eer ,!en a %a"netic su*stance

    li6e iron is $laced in t!e field t!e %a"netic field lines

     *eco%e concentrated0

    B T!is a*ilit) of a su*stance to concentrate %a"netic flu4 iscalled $er%ea*ilit)0 A %a"netic field can *e created *) a

     $er%anent %a"net or an electro%a"net ,!ic! is a loo$ed

    coil of conductin" %aterial ,ound on a core %an) ti%es0

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    Inductance

     T!e (self inductance ' is an indication of t!e a*ilit) of a

    coil to o$$ose an) c!an"e in current flo,in" t!rou"! t!e

    coil0 T!e inductance ' of a c)lindrical coil is "ien *)

    ?!ere ' is t!e inductance Henr) HF

      G is t!e $er%ea*ilit) of t!e core H@%F

      n is t!e nu%*er of turns of coil  A is t!e cross sectional area of core %/F

      l is t!e len"t! of core %F

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    Inductie transducers

      Inductie transducers are t!ose in ,!ic! SE'>

    IN#UCTANCE of a coil or t!e MUTUA' IN#UCTANCE

    of a $air of coil is altered due to ariation in t!e

    %easurand0 C!an"e in inductance ' is %easured0 T!e self inductance of a coil refers to t!e flu4 lin6a"e

    ,it!in t!e coil due to current in t!e sa%e coil0

     Mutual inductance refers to t!e flu4 lin6a"es in a coil

    due to current in ad+acent coil0

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    Inductie transducers

    T!e self inductance  of a coil refers to t!e flu4 lin6a"e

    ,it!in t!e coil due to current in t!e sa%e coil0

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    Inductie transducers

    Mutual inductance  refers to t!e flu4 lin6a"es in a coil

    due to current in ad+acent coil0

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    Inductie transducers

    • Consider a set of t,o coils s!arin" t!e sa%e core i0e0 a

    transfor%er *asicall)0 Note t!at one of t!e coil ($ri%ar)coil is drien *) a $o,er source ,!ile t!e ot!er

    (secondar) coil $roduces a olta"e induced fro% t!e

     $ri%ar) coil0

    B T!e olta"e on t!e secondar) coil de$ends on %utual

    inductance *et,een t!e t,o coils0 If t!e core is %ade

    %oa*le in res$onse to t!e dis$lace%ent of a tar"et o*+ect

    t!e %utual inductance ,ill c!an"e resultin" in a olta"e

    c!an"e in t!e secondar) coil0

    • Usin" t!is $rinci$le t!e '#T and R#T ,or6s0

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    Inductie transducers

    • In t!e %a"netic circuits reluctance is e3uialent to resistance

    and de$ends on

      Nu%*er of turns

     Area of cross section of ,ire .er%ea*ilit) of t!e %ediu%

    •  Air !as %uc! lo,er $er%ea*ilit) t!an a ferro%a"netic

    %aterial0

    • Introducin" air "a$ is li6e introducin" !i"! resistance0

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    Inductie transducers

    • In t!e %a"netic circuits reluctance is e3uialent to resistance

    and de$ends on

      Nu%*er of turns

     Area of cross section of ,ire

     .er%ea*ilit) of t!e %ediu%

    •  Air !as %uc! lo,er $er%ea*ilit) t!an a ferro%a"netic

    %aterial0

    • Introducin" air "a$ is li6e introducin" !i"! resistance0

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    Inductie transducers

    • Air Cored Coils

    Can *e o$erated at !i"!er

    fre3uencies *ecause t!ereare no edd) current losses

    in air core0

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    Inductie transducers

    • Iron cored coils

     Inductance de$ends on

    t!e alue of current0

     At !i"! fre3uencies

    edd) current losses are

    !i"!0

     Si7e %uc! s%aller t!an

    air cored0

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    Linear Variable-Differential Transformer(LVDT)

    •  T!e t,o secondar) coils are connected in t!e o$$osite

     $!ase0• ?!en t!e core is in t!e %iddle t!ere is no out$ut olta"e0

    • Moin" t!e core fro% t!e central $osition un*alances t!esecondar)Js deelo$in" an out$ut0

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    Linear Variable-Differential Transformer(LVDT)

     Applications: To %easure linear dis$lace%ent e0"0 for%easurin" tu*e len"t!s in a steel $lant a$$lied in linearsero%ec!anis%s etc0

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    'inear aria*le-#ifferential

    Transfor%er ('#T

    -x

    Vo=V1-V2

    Vi

    V1 V2

    V1 > V2 Vi

    Vo

    '#Ts are deices to %easure

    dis$lace%ent *) %odif)in" s$atialdistri*ution of an alternatin"

    %a"netic field0

    Oscillating excitation voltage-5 !" to 25 #!"

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    'inear aria*le-#ifferential Transfor%er

    ('#T

    $=

    Vo=V1-V2

    Vi

    V1 V2

    V2 = V1

    Vi

    Vo

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    'inear aria*le-#ifferential Transfor%er

    ('#T

    %x

    Vo=V1-V2

    Vi

    V1 V2

    V2 > V1

    Vi

    Vo

    &o' te irection of is*lacement can be etermine from te relative *ase of te

    signal+

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    Linear Variable Diferential

     Trans!r"er #LVDT$

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    •  T!e s$an ran"es fro%

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    A rotar) aria*le differential transfor%er(R#T

      A rotar) aria*le differential transfor%er (R#T isfor %easurin" an"ular dis$lace%ents and

    o$erates in t!e sa%e %anner as a '#T0

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     , ca*acitor is an electrical com*onent ic

    essentiall. consists of to *lates se*arate

    b. an ins/lator+Te *ro*ert. of a ca*acitor to store an

    electric carge en its *lates are at ifferent

    *otential is referre to as ca*acitance+

    CA.ACITIE TRANS#UCERS

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    0f te ca*acitance is large more carge is

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    d

    AC

      r <εε

    =

    +

    0f te ca*acitance is large' more carge is

    neee to establis a given voltage ifference+

    Te ca*acitance beteen to *arallel metallic

    *lates of area

       

       ×=   −

    m

     F 1/<

      1

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    10 Circular %otion %easure%ent• Aaila*le in arious si7es and resolutions

    • Used in co%$uter %ouse rollers

    /0 Co%$onents• Circular dis6 ,it! slots

    • #iode and $!oto sensor 

    • #i"ital circuitr) to $rocess $ulses

    Incre%ental O$tical Encoders

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    %!r&in' (rin)i(le

    Ligt so/rce' ioe

    *oto sensor 

    •1 f/ll *inc is e/ivalent to one f/ll c.clemae b. te trans*arent an o*a/e

    inos

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    t,

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    +)!nt,.

    oto sensor 

    ioe

    oto sensor 

    ioe

    •3otating is#

    blocking ligt

    •oto sensor as a

    low logic o/t*/t

    •3otating is#

    allowing ligt tro/g

    •oto sensor as a 

    high logic o/t*/t

    •4ontin/o/s train of */lses forme as te *oto sensor traverses

    beteen logic ig an logic lo in res*onse to te rotation of te is#

    Logical Logical 1

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    10 O$tical incre%ental encoder is used to %easure

    10 .osition

    /0 elocit)

    0 #irection of rotation/0 No need for ot!er A@# circuits

    10 Out$uts can *e directl) fed to

      %icro$rocessor@%icrocontroller 

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    Absolute Optical Encoder working

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    Absolute Optical Encoder working

    • A disc or a $late containin"o$a3ue and trans$arent se"%ents $asses *et,een a li"!t source(suc! an 'E# and detector tointerru$t a li"!t *ea%0

    • T!e electronic si"nals t!at are"enerated are t!en fed into t!econtroller ,!ere $osition and

    elocit) infor%ation iscalculated *ased u$on t!e si"nalsreceied

    05/03/16 09:05 AM &al*an

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    A*solute O$tical Encoder

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    A*solute O$tical Encoder 

    • In t!e fi" ,ord si7e of data is 2*its0

    • Outer%ost Ele%ent is 'S=0• Inner%ost Ele%ent is MS=0• T!e An"ular $osition is "ien as8

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    'inear Encoder Codes

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    Reca$

      To$ics dealt ,it! in t!is class•  Classification of transducers•  #is$lace%ent transducers

    •  resistance *ased transducers $otentio%eter 

    •  Inductie transducers '#T•  Ca$acitie transducers•  Non contact $osition sensors O$tical Encoders