A new ALE formulation for sloshing analysis

Arbitrary Lagrangian Eulerian finite element methods gain interest for the capability to control mesh geometry independently from material geometry, the ALE methods are used to create a new undistorted mesh for the fluid domain. In this paper we use the ALE technique to solve fuel slosh problem. Fuel slosh is an important design consideration not only for the fuel tank, but also for the structure supporting the fuel tank. "Fuel slosh" can be generated by many ways: abrupt changes in acceleration (braking), as well as abrupt changes in direction (highway exit-ramp). Repetitive motion can also be involved if a "sloshing resonance" is generated. These sloshing events can in turn affect the overall performance of the parent structure. A finite element analysis method has been developed to analyze this complex event. A new ALE formulation for the fluid mesh has been developed to keep the fluid mesh integrity during the motion of the tank. This paper explains the analysis capabilities on a technical level. Following the explanation, the analysis capabilities are validated against theoretical using potential flow for calculating fuel slosh frequency.

[1]  D. Benson Computational methods in Lagrangian and Eulerian hydrocodes , 1992 .

[2]  B. V. Leer,et al.  Towards the ultimate conservative difference scheme. IV. A new approach to numerical convection , 1977 .

[3]  B. V. Leer,et al.  Towards the Ultimate Conservative Difference Scheme , 1997 .

[4]  Jin-Rae Cho,et al.  Baffled fuel-storage container: parametric study on transient dynamic characteristics , 2002 .

[5]  David J. Benson,et al.  Eulerian finite element methods for the micromechanics of heterogeneous materials: Dynamic prioritization of material interfaces , 1998 .

[6]  L YoungsD,et al.  Time-dependent multi-material flow with large fluid distortion. , 1982 .

[7]  T. Nakayama,et al.  AN EULERIAN FINITE ELEMENT METHOD FOR TIME‐DEPENDENT FREE SURFACE PROBLEMS IN HYDRODYNAMICS , 1996 .

[8]  D. Benson A mixture theory for contact in multi-material Eulerian formulations , 1997 .

[9]  T. Belytschko,et al.  A uniform strain hexahedron and quadrilateral with orthogonal hourglass control , 1981 .

[10]  David J. Benson,et al.  Momentum advection on a staggered mesh , 1992 .

[11]  P. Woodward,et al.  The numerical simulation of two-dimensional fluid flow with strong shocks , 1984 .

[12]  J. Zolésio,et al.  Arbitrary Lagrangian–Eulerian and free surface methods in fluid mechanics , 2001 .

[13]  Wing Kam Liu,et al.  Lagrangian-Eulerian finite element formulation for incompressible viscous flows☆ , 1981 .

[14]  C. W. Hirt,et al.  YAQUI: an arbitrary Lagrangian--Eulerian computer program for fluid flow at all speeds , 1973 .

[15]  M. Souli,et al.  ALE formulation for fluid–structure interaction problems , 2000 .

[16]  R. Blevins,et al.  Formulas for natural frequency and mode shape , 1984 .