A time semi-implicit scheme for the energy-balanced coupling of a shocked fluid flow with a deformable structure
被引:7
作者:
Puscas, Maria Adela
论文数: 0引用数: 0
h-index: 0
机构:
Univ Paris Est, CERMICS ENPC, F-77455 Marne La Vallee, France
CEA, DAM, DIF, F-91297 Arpajon, France
CNRS, LIMSI, F-91403 Orsay, FranceUniv Paris Est, CERMICS ENPC, F-77455 Marne La Vallee, France
Puscas, Maria Adela
[1
,2
,3
]
论文数: 引用数:
h-index:
机构:
Monasse, Laurent
[1
]
Ern, Alexandre
论文数: 0引用数: 0
h-index: 0
机构:
Univ Paris Est, CERMICS ENPC, F-77455 Marne La Vallee, FranceUniv Paris Est, CERMICS ENPC, F-77455 Marne La Vallee, France
Ern, Alexandre
[1
]
Tenaud, Christian
论文数: 0引用数: 0
h-index: 0
机构:
CNRS, LIMSI, F-91403 Orsay, FranceUniv Paris Est, CERMICS ENPC, F-77455 Marne La Vallee, France
Tenaud, Christian
[3
]
Mariotti, Christian
论文数: 0引用数: 0
h-index: 0
机构:
CEA, DAM, DIF, F-91297 Arpajon, FranceUniv Paris Est, CERMICS ENPC, F-77455 Marne La Vallee, France
Mariotti, Christian
[2
]
Daru, Virginie
论文数: 0引用数: 0
h-index: 0
机构:
CNRS, LIMSI, F-91403 Orsay, France
Ensam, Lab DynFluid, F-75013 Paris, FranceUniv Paris Est, CERMICS ENPC, F-77455 Marne La Vallee, France
Daru, Virginie
[3
,4
]
机构:
[1] Univ Paris Est, CERMICS ENPC, F-77455 Marne La Vallee, France
The objective of this work is to present a conservative coupling method between an inviscid compressible fluid and a deformable structure undergoing large displacements. The coupling method combines a cut-cell Finite Volume method, which is exactly conservative in the fluid, and a symplectic Discrete Element method for the deformable structure. A time semi-implicit approach is used for the computation of momentum and energy transfer between fluid and solid, the transfer being exactly balanced. The coupling method is exactly mass-conservative (up to round-off errors in the geometry of cut-cells) and exhibits numerically a long-time energy-preservation for the coupled system. The coupling method also exhibits consistency properties, such as conservation of uniform movement of both fluid and solid, absence of numerical roughness on a straight boundary, and preservation of a constant fluid state around a wall having tangential deformation velocity. The performance of the method is assessed on test cases involving shocked fluid flows interacting with two and three-dimensional deformable solids undergoing large displacements. (C) 2015 Elsevier Inc. All rights reserved.