2008
DOI: 10.1016/j.jsv.2008.03.022
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Dynamics of a rectangular plate resting on an elastic foundation and partially in contact with a quiescent fluid

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Cited by 47 publications
(18 citation statements)
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“…Applying the method of separation of variables based on the boundary conditions of Eqs. (11)(12)(13)(14)(15)(16)(17)(18)(19), general solution of Eq. (10) is given as…”
Section: Formulation Of the Fluid Oscillationsmentioning
confidence: 99%
See 1 more Smart Citation
“…Applying the method of separation of variables based on the boundary conditions of Eqs. (11)(12)(13)(14)(15)(16)(17)(18)(19), general solution of Eq. (10) is given as…”
Section: Formulation Of the Fluid Oscillationsmentioning
confidence: 99%
“…Numerous studies have been performed to investigate free and forced vibrations of thin isotropic plates in partial contact with a fluid. Some of the most complete reviews on the subject are presented by Khorshidi [1], Amabili [2,3], Pellicano and Amabili [4], Jeong and Kim [5], Jeong et al [6,7], Kwak [8], Zhou and Cheung [9], Chang and Liu [10], Ergin and Ugurlu [11], Zhou and Liu [12], Ugurlu et al [13] and Kerboua et al [14].…”
Section: Introductionmentioning
confidence: 99%
“…According to this technique, the M th term approximate solution of (2), (8) is sought in the form (9) where ( ) i Q t are coordinates in modal space and ( ) i P x are the normal modes of vibration written as (10) No difficulty arises at all to show that for a beam with simply supported end conditions, taking into account equation (10), equation (9) can be written as (11) Substituting equation (11) into the governing equation (8), one obtains (12 ) which after some simplifications and rearrangements yields (13) To determine the expression for ( ) i Q t , the expression on the LHS of equation (13) is required to be orthogonal to the function . Thus, multiplying equation (13) by and integrating with respect to x from x=0 to x=L, leads to (14) where , , (16) and considering only the i th particle of the system, equation (14) can then be written as (17) where , and (18) To obtain the solution of the equation (17), it is subjected to a Laplace transform defined as (19) where s is the Laplace parameter.…”
Section: Solution Proceduresmentioning
confidence: 99%
“…When these important engineering structures are resting on an elastic foundation, the structure-foundation interaction effects play significant roles in their response behaviour and alter the dynamic states of B. Omolofe a T.O. Adeloye the structures from those vibrating in the absence of foundation [Ugurlu et al (2008)]. Hence, the dynamic behaviour of structures on elastic foundation is of great importance in structural, aerospace, civil, mechanical and marine engineering applications.…”
Section: Introductionmentioning
confidence: 99%