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    Calculation of the Response of an Impulsively Excited Oscillator in an Infinite Acoustic Fluid

    Source: Journal of Applied Mechanics:;1981:;volume( 048 ):;issue: 004::page 749
    Author:
    A. V. Clark
    ,
    A. M. Whitman
    DOI: 10.1115/1.3157727
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: The response of an impulsively excited single-degree-of-freedom oscillator submerged in an infinite acoustic fluid is considered. The character of the response is determined by the quantity ka; k is the wave number associated with the in-vacuo natural frequency of the oscillator, and a is a characteristic structural dimension. For low-frequency oscillators (ka ≪ 1), the response consists of two parts. The first is the usual hydrodynamic solution in which the effect of the fluid on the structure is that of an added mass. The second is much smaller (of order ka) and is significant only in a “boundary layer” in time of order a/c, with c the fluid sonic velocity. For high-frequency oscillators (ka ≫ 1), the principal effect of the fluid is a decay of oscillator vibration due to sound radiation.
    keyword(s): Acoustics , Fluids , Radiation (Physics) , Dimensions , Sound , Waves , Boundary layers AND Vibration ,
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      Calculation of the Response of an Impulsively Excited Oscillator in an Infinite Acoustic Fluid

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    http://yetl.yabesh.ir/yetl1/handle/yetl/94021
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    • Journal of Applied Mechanics

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    contributor authorA. V. Clark
    contributor authorA. M. Whitman
    date accessioned2017-05-08T23:10:08Z
    date available2017-05-08T23:10:08Z
    date copyrightDecember, 1981
    date issued1981
    identifier issn0021-8936
    identifier otherJAMCAV-26188#749_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/94021
    description abstractThe response of an impulsively excited single-degree-of-freedom oscillator submerged in an infinite acoustic fluid is considered. The character of the response is determined by the quantity ka; k is the wave number associated with the in-vacuo natural frequency of the oscillator, and a is a characteristic structural dimension. For low-frequency oscillators (ka ≪ 1), the response consists of two parts. The first is the usual hydrodynamic solution in which the effect of the fluid on the structure is that of an added mass. The second is much smaller (of order ka) and is significant only in a “boundary layer” in time of order a/c, with c the fluid sonic velocity. For high-frequency oscillators (ka ≫ 1), the principal effect of the fluid is a decay of oscillator vibration due to sound radiation.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleCalculation of the Response of an Impulsively Excited Oscillator in an Infinite Acoustic Fluid
    typeJournal Paper
    journal volume48
    journal issue4
    journal titleJournal of Applied Mechanics
    identifier doi10.1115/1.3157727
    journal fristpage749
    journal lastpage752
    identifier eissn1528-9036
    keywordsAcoustics
    keywordsFluids
    keywordsRadiation (Physics)
    keywordsDimensions
    keywordsSound
    keywordsWaves
    keywordsBoundary layers AND Vibration
    treeJournal of Applied Mechanics:;1981:;volume( 048 ):;issue: 004
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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