ME 598 – Project

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    ME 598 – Noise in Engineering andPhysical Systems

    Project Presentation by

    Bharath Raghavan

    Fall !"5

    Acceleration waves in

    random media

    "

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    Acceleration waves

    • #cceleration $aves are moving sing%lars%r&aces $ith a j%m' in 'article acceleration(

    • )se&%l &or st%dying the &ormation o&shoc*$aves

    •  +hey are governed by the Berno%lli e,%ation

    - is 'osition. / is the j%m' in 'articleacceleration. 0 and 1 re'resent the dissi'ationand elastic nonlinearity o& the material(

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    Acceleration waves inhomogeneous media

    •  +here e-ists a 2nite distance in $hicha shoc* can be &ormed

    •   is the critical am'lit%de. and isthe initial am'lit%de

    • 3& 4 then the $ave decayse-'onentially

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    Acceleration waves in Randommedia

    "( Se'aration o& Scales –  +he $ave&ront thic*ness is 6

     – 7haracteristic grain sie is d

    ( 7ase " – 6 d : ;eterministic contin%%m limit

     – Fl%ct%ations are insigni2cant as the$ave&ront is oblivio%s to local materialdisorder

    ( 7ase  – 6 is 2nite relative to grain sie

     – Fl%ct%ations are signi2cant

    ?

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    Acceleration waves in Randommedia

    • 3nterested in Case (2).

    5

    Fig 1. 6d a deterministic contin%%m . 6 is2nite relative to d so statistical @%ct%ations are

    signi2cant(

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    Stochastic BernoulliEquation

    •  +he case $here 0 and 1 are'ert%rbed by the same standarderoAmean $hite noise

    • #dmit the &ollo$ing decom'osition

    • $here S is the intensity val%e(D

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    Stochastic BernoulliEquation

    • S%bstit%ting the decom'osition in theBerno%lli ;E gives.

    • e inter'ret the above e,%ation in theStratonovich sense to obtain the S;E

    • $here is the Stratonovich ty'ediGerential o& the einer 'rocess

    H

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    Equivalent to S!E•

    e $ish to %se the to "ormula tocom'%te vario%s &%nctions o& /(

    • So $e need to get the e,%ivalent 3to

    S;E &or the Stratonovich S;E(• e de2ne

    • +o obtain

    8

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    Equivalent to S!E

    • e de2ne the 3to S;E as

    $here

    9

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    #oments equations•

    e are 'rimarily interested in themoments so $e de2ne

    #nd a''lying 3toIs &orm%la

    •  +a*ing the e-'ectation

    "!

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    $he inverse am%litude

    •  +he inverse am'lit%de is de2ned as

    • 3t trans&orms the Jblo$A%'I o& the$ave am'lit%de / to in&nit' to oneo" erocrossing

    •  #''lying 3toIs &orm%la

    ""

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    • e obtain

    Sim'li2ed to

    Moments e,%ation – via thes%bstit%tion

    "

    $he inverse am%litude

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    $he inverse am%litude

    • Set o& e,%ations &or moments

    • First moments

    "

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    #oments o" the inverseam%litude

    • #nalytical e-'ressions &or &rst andsecond moment

    $here

    "?

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    #ean o" the inverseam%litude

    • Set

    • e are interested in 2nding thecritical am'lit%de

    • #lso and

    "5

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    Critical Am%litude

    • 7ase ":

     – No shoc* &ormation as and

    • 7ase :

     – JBlo$ %'I as and•  +he critical inverse am'lit%de is

    given as

    "D

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    7oncl%sions

    • bservations: +he stochastic criticalam'lit%de is in general less than thedeterministic critical am'lit%de

    • #dditional St%dies: – Stochastic Berno%lli e,%ation $ith t$o

    inde'endent $hite noise 'ert%rbations

     –

     Stochastic Berno%lli e,%ation $ith t$ocorrelated $hite noise 'ert%rbations

     – Fo**erAPlanc* e,%ation and 'robability o&shoc* &ormation

    "H