Multidimensional modal analysis of nonlinear sloshing in a rectangular tank with finite water depth
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Cites background or methods from "Multidimensional modal analysis of ..."
...A multimodal algorithm should be used [11]....
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...16 represents an off-resonance case [11,21] with a forcing frequency higher than the first natural sloshing frequency (xh=x1 1⁄4 1:283), similar to...
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...[11], Ockendon and Ockendon [31], Hill [21]....
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...The role of critical depth in tanks subjected to horizontal motions have also been studied [10–13,21]....
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...[20], Faltinsen [11], Waterhouse [41] found hc=k 1⁄4 0:583 m or in general hc 1⁄4 0:337 b for the first mode, respectively....
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216 citations
References
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"Multidimensional modal analysis of ..." refers background or methods in this paper
...Multidimensional modal analysis of nonlinear sloshing 203 (see Shemer 1990 and Tsai, Yue & Yip 1990) or a system of four first-order ordinary differential equations for a vertical circular cylindrical tank (see Miles (1984a, b)). Funakoshi & Inoue (1991) used Miles’ model in their detailed simulations....
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...The canonical formulation of this principle is given by Bateman (1944) and Luke (1967) (for gravity surface waves in infinite basins)....
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...Multidimensional modal analysis of nonlinear sloshing 203 (see Shemer 1990 and Tsai, Yue & Yip 1990) or a system of four first-order ordinary differential equations for a vertical circular cylindrical tank (see Miles (1984a, b)). Funakoshi & Inoue (1991) used Miles’ model in their detailed simulations. The averaging technique and small-dimensional modal modelling complement each another in the analysis of the steady-state free surface response due to periodic tank excitations. But these methods are questionable in modelling coupled fluid–structure interaction with complicated non-periodic tank motions when transient effects matter. These complex motions are simulated in engineering applications either numerically or by phenomenological (usually pendulum) models (see Chapter 5 of Narimanov et al. 1977 or Pilipchuk & Ibrahim 1997). An alternative is to use Narimanov’s original technique with the modal representation in the form (1.1) and more general asymptotic assumptions of βi and Rn in order to reach reasonable dimensions of the modal systems. The successful use of this approach is reported by Limarchenko & Yasinsky (1997) and Lukovsky & Timokha (1995) for simplified models of spacecraft....
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336 citations
"Multidimensional modal analysis of ..." refers background or methods or result in this paper
...The general form of a discrete infinite-dimensional modal system is derived in the first part of this paper by the Bateman–Luke (pressure-integral Lagrangian) variational principle. This idea was proposed independently by Miles (1976) and Lukovsky (1976). They studied forced small-amplitude translatory motions of a vertical circular cylindrical tank. The surfacemodes and domainmodes were obtained by linear theory and related by (1.2). Our derivation of a discrete infinite-dimensional modal system is not restricted to a particular type of body motion. The surface and domain modes are not associated with natural modes and no asymptotic assumptions are introduced in the first stage of the derivation. The infinite-dimensional modal system can be reduced to a finite-dimensional form by assuming small-amplitude forced oscillations and associate order of magnitudes of the different modes. This is done in the second part of the paper to analyse nonlinear sloshing in a two-dimensional rectangular smooth tank with finite water depth. Both forced translatory and rotational body motions are considered. The lowest natural mode is assumed to dominate and the three lowest modes interact nonlinearly with each other. Several modes having higher order are considered by linear theory. The asymptotic theory constructed is a special multidimensional analogue of the model by Ikeda & Nakagawa (1997) and the direct generalization of the third-order hydrodynamic theory by Faltinsen (1974). Experiments on nonlinear sloshing caused by primary mode resonant excitation have been conducted....
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...The general form of a discrete infinite-dimensional modal system is derived in the first part of this paper by the Bateman–Luke (pressure-integral Lagrangian) variational principle. This idea was proposed independently by Miles (1976) and Lukovsky (1976). They studied forced small-amplitude translatory motions of a vertical circular cylindrical tank. The surfacemodes and domainmodes were obtained by linear theory and related by (1.2). Our derivation of a discrete infinite-dimensional modal system is not restricted to a particular type of body motion. The surface and domain modes are not associated with natural modes and no asymptotic assumptions are introduced in the first stage of the derivation. The infinite-dimensional modal system can be reduced to a finite-dimensional form by assuming small-amplitude forced oscillations and associate order of magnitudes of the different modes. This is done in the second part of the paper to analyse nonlinear sloshing in a two-dimensional rectangular smooth tank with finite water depth. Both forced translatory and rotational body motions are considered. The lowest natural mode is assumed to dominate and the three lowest modes interact nonlinearly with each other. Several modes having higher order are considered by linear theory. The asymptotic theory constructed is a special multidimensional analogue of the model by Ikeda & Nakagawa (1997) and the direct generalization of the third-order hydrodynamic theory by Faltinsen (1974)....
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...The derivation is based on the Bateman–Luke variational principle. The free surface motion and velocity potential are expanded in generalized Fourier series. The derived infinite-dimensional modal system couples generalized time-dependent coordinates of free surface elevation and the velocity potential. The procedure is not restricted by any order of smallness. The general multidimensional structure of the equations is approximated to analyse sloshing in a rectangular tank with finite water depth. The amplitude–frequency response is consistent with the fifth-order steady-state solutions by Waterhouse (1994). The theory is validated by new experimental results....
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...The canonical formulation of this principle is given by Bateman (1944) and Luke (1967) (for gravity surface waves in infinite basins)....
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...We will use a Bateman–Luke variational principle and introduce the pressure in the Lagrangian of the Hamilton principle. The idea of the pressure integral as the Lagrangian in hydrodynamic problems was first proposed by Hargneaves (1908). The canonical formulation of this principle is given by Bateman (1944) and Luke (1967) (for gravity surface waves in infinite basins)....
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218 citations
"Multidimensional modal analysis of ..." refers background or methods or result in this paper
...It is also necessary that the water depth is not shallow and the fluid does not hit the tank ceiling (see, also, physical arguments presented in Faltinsen 1974 and the book by Mikishev 1978)....
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...The asymptotic theory constructed is a special multidimensional analogue of the model by Ikeda & Nakagawa (1997) and the direct generalization of the third-order hydrodynamic theory by Faltinsen (1974)....
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...This was demonstrated by Solaas & Faltinsen (1997), where Moiseev’s theory was applied to two-dimensional sloshing....
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...It is assumed, as in the theory by Faltinsen (1974), that O(β31 ) = O(H) = O(ψ0) = ....
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...The branches presented differ from diagrams obtained by Faltinsen’s theory only for large values of |A|/l and far away from the main resonance σ̄1 = 1. The last difference is due to the change of m1 when varying σ. The results agree with the fifth-order theory by Waterhouse (1994) for sufficiently small amplitudes....
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189 citations
"Multidimensional modal analysis of ..." refers methods in this paper
...The derivation of the modal system from the original free boundary problem was first proposed by Narimanov (1957) based on a perturbation technique. It has been further developed by Dodge, Kana & Abramson (1965), Narimanov, Dokuchaev & Lukovsky (1977) and Lukovsky (1990)....
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...The derivation of the modal system from the original free boundary problem was first proposed by Narimanov (1957) based on a perturbation technique....
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...This idea was proposed independently by Miles (1976) and Lukovsky (1976)....
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...Using the Bateman–Luke variational principle, we generalize the procedure proposed by Miles (1976) and Lukovsky (1976) to derive a modal system describing nonlinear sloshing of an incompressible perfect fluid with irrotational flow partly occupying a tank performing an arbitrary three-dimensional…...
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