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Most of the tanks are smooth inside and the resulting small uid dynamic damping of the system is very small, thus increasing the slosh- ing amplitudes

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G. Fotia 1

M. Landrini 2

1CRS4, Center for Advanced Studies, Research and Development in Sardinia, Cagliari, Italy

2INSEAN, The Italian Ship Model Basin, Roma, Italy.

Sloshing ows, i.e. resonant uid motion in con- ned domains, play a signi cant role in many practi- cal circumstances. Early work relevant to this topic is reported e.g. in [1]. In the eld of naval hy- drodynamics, ship response to incoming waves can excite violent motions of transported liquids (crude oil, gas, etc.). Most of the tanks are smooth inside and the resulting small uid dynamic damping of the system is very small, thus increasing the slosh- ing amplitudes. On this ground, large oscillatory structural loads are expected, as well as local im- pulsive loads (slamming) on lateral walls (in case of small lling level) or on the tank roof (for higher lling heights).

Accurate prediction of sloshing loads is of main concern during the design stage of ship tanks. In most of the applications, the dynamic interaction between the structural vibrations and the ow eld is neglected, i.e. uid loads are determined by studying liquid sloshing in rigid tanks. However, the accuracy of this simpli ed analysis is question- able when dealing with lighter structures or high- strength structural steels. This latter case is of growingly importance in current design practice, and the modeling of uid-structure interaction is needed to understand the various hydroelastic phe- nomena and to assess the safety of the system.

The scope of the presentation is to review our on- going e ort in developing a simulation tool to de- scribe the coupled structural- uid dynamic system.

The adopted uid-structure model consist of three components: a uid dynamics solver, a structural dynamic solver, and an interaction model along the uid-structure interface, see e.g. [6, 3]. More pre- cisely, by virtue of the high Reynolds number typi- cally encountered in practical applications, the ow eld is described through an inviscid model. Non- linear free surface motions are allowed, though a linearized version of the problem will be used as a test case against available analytical solution. Lin- ear elasticity theory is used to describe the dynamic behavior of the exible tank.

To handle unsteady free-surface motions typically encountered in sloshing ows we employ an high or- der boundary element method based on B-Spline representation [5]. This method is well suited to handle standing waves and impulsive free-surface motions. A semi-discrete nite element formula- tion for the structural dynamic equation of motion is used for the exible walls of the tank.

Starting from a variationalformulationof the cou- pled problem [8], we investigate some possible algo- rithms to solve the full unsteady interaction phe- nomenon.

Many di erent schemes from fully implicit to fully explicit can be used for the time discretization of the problem [4, 2, 7]. Relevant merits and disadvantages of the various possible approach for the problem at hand will be presented and discussed. Issues related to the stability and the accuracy of the numerically coupled simulations will also be examined with the objective of identifying a stable, accurate and e- cient algorithm to solve the coupled sloshing prob- lem.Finally, some initial results on a fully explicit in- teraction two-dimensional model problem will be presented.

References

[1] H.N. Abramson, ed. The dynamic behavior of liquids in moving containers with applications to space vehicle technology. Technical Report NASA-SP-106, NASA, 1966.

[2] J.R. Cebral and R. Lohner. Fluid-structure cou- pling: Extensions and improvements. Report AIAA-97-064, AIAA, 1997.

[3] G. Fotia and G. Siddi. Transient dynamic re- sponse of a large telescope antenna under wind loading: 3D uid-structure computation. InEx- tended Abstracts of the ASI Workshop "The Sar- dinian Radiotelescope from Science to Space", Porto Cervo, Italy, May 1999.

[4] C. Grandmont. Analyse mathematique et nu- merique de quelques problemes d'interaction uide-structure. PhD thesis, Universite Paris 6, 1998.

[5] M. Landrini, G. Grytyr, and O.M. Faltinsen.

A B-spline based BEM for unsteady free surface ows. Journal of Ship Research, 1:1{12, 1999.

[6] K. Stein, R. Benney, V. Kalro, T. Tezdu- yar, J. Leonard, and M. Accorsi. Parachute uid-structure interactions: 3D computation.

Preprint 98-052, AHPCRC, 1998.

[7] P. Le Tallec and J. Mouro. Structures en grands deplacements couplees a des uides en mouve- ment. Rapport de Recherche 2961, INRIA, 1996.

[8] L.L. Thomson. Design and analysis of space- time and Galerkin/least-squares nite element methods for uid-structure interaction in exte- rior domains. PhD thesis, Department of Me- chanical Engineering, Stanford University, 1994.

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