1992
DOI: 10.1007/bf00850629
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Three-dimensional bent-gravity waves with non-uniform compression

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Cited by 9 publications
(2 citation statements)
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“…We will consider the layer of an ideal incompressible heavy fluid of thickness H which occupies the domain , , , where x and y are the horizontal coordinates and z is the vertical coordinate directed upward. A thin elastic plate floating on the upper boundary of fluid can be described by the Kirchhoff-Love model with regard to the longitudinal, transverse and shear compressive forces [7,8]. Initially, the fluid and the plate are at rest but, starting from the instant t = 0, a time-dependent specified external pressure begins to act on the plate.…”
Section: Formulation Of the Problemmentioning
confidence: 99%
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“…We will consider the layer of an ideal incompressible heavy fluid of thickness H which occupies the domain , , , where x and y are the horizontal coordinates and z is the vertical coordinate directed upward. A thin elastic plate floating on the upper boundary of fluid can be described by the Kirchhoff-Love model with regard to the longitudinal, transverse and shear compressive forces [7,8]. Initially, the fluid and the plate are at rest but, starting from the instant t = 0, a time-dependent specified external pressure begins to act on the plate.…”
Section: Formulation Of the Problemmentioning
confidence: 99%
“…Three types of forces are possible in the three-dimensional case, namely, these are longitudinal, transverse and shear forces [5]. The behavior of free flexural-gravity waves in the presence of non-uniform compression was studied in [6] and the steady-state wave motion under the action of an external load was considered in [7]. The results of both studies were also given in monograph [8].…”
mentioning
confidence: 99%