2011
DOI: 10.1017/jfm.2011.161
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On the coupled time-harmonic motion of water and a body freely floating in it

Abstract: We consider a spectral problem that describes the time-harmonic small-amplitude motion of the mechanical system that consists of a three-dimensional water layer of constant depth and a body (either surface-piercing or totally submerged), freely floating in it. This coupled boundary-value problem contains a spectral parameter – the frequency of oscillations – in the boundary conditions as well as in the equations governing the body motion. It is proved that the total energy of the water motion is finite and the… Show more

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Cited by 15 publications
(23 citation statements)
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“…This paper continues the rigorous study (initiated in [3]) of a freely floating rigid bodies trapping time-harmonic waves in an inviscid, incompressible, heavy fluid, say water (see also [6,7,8] and [4]). We consider the infinitely deep water in irrotational motion bounded from above by a free surface unbounded in all horizontal directions, but unlike the cited papers dealing with the open surface, we assume here that it is totally covered with the brash ice.…”
Section: Introductionmentioning
confidence: 58%
“…This paper continues the rigorous study (initiated in [3]) of a freely floating rigid bodies trapping time-harmonic waves in an inviscid, incompressible, heavy fluid, say water (see also [6,7,8] and [4]). We consider the infinitely deep water in irrotational motion bounded from above by a free surface unbounded in all horizontal directions, but unlike the cited papers dealing with the open surface, we assume here that it is totally covered with the brash ice.…”
Section: Introductionmentioning
confidence: 58%
“…In the same way as in Kuznetsov & Motygin (2011, 2012, this yields the following assertion about the kinetic and potential energy of the water motion. that is, ϕ ∈ H 1 (W).…”
Section: Equipartition Of Energymentioning
confidence: 71%
“…This paper continues the rigorous study (initiated in Kuznetsov 2011) of the coupled time-harmonic motion of a freely floating rigid body and an inviscid, incompressible, heavy fluid, say water; see also Kuznetsov & Motygin (2011, 2012, 2015 and Kuznetsov (2015). We consider infinitely deep water in irrotational motion, bounded from above by a free surface unbounded in all horizontal directions, but unlike the cited papers dealing with the open surface, we assume here that it is totally covered with brash ice.…”
Section: Introductionmentioning
confidence: 93%
“…As in Theorem 4.3, the velocity potential ϕ m satisfies relations (7) and (8), whereas the boundary condition (9) holds on every S k in view of the way how these surfaces are constructed using the displacement vectors (31). It remains to verify 6N equations (10) of which 5N take the same form as equalities (27) with the exception of the first one. The latter is as follows:…”
Section: Modified Stream Functions and Heaving Trapping Structuresmentioning
confidence: 99%