2006
DOI: 10.1007/s00466-006-0100-7
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A 3D implicit unstructured-grid finite volume method for structural dynamics

Abstract: In this work, a new vertex-based finite volume method (FVM) using unstructured grids and cell-based data structure is proposed for computational analysis of two-and three-dimensional (2D/3D) general structural dynamic problems. The governing equations are spatially discretized by the FVM and an implicit dual time stepping scheme is employed to integrate the equations in time. The proposed method is applied to calculate deformations and dynamics of 2D and 3D cantilevers, as well as simply supported and clamped … Show more

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Cited by 17 publications
(13 citation statements)
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“…The governing equation for a continuum undergoing motion is given by Cauchy’s equation in three dimensions60, 61: ρνit=·σij+fi where the subscript i is a free index as before, f i is the external force, and v i is the velocity of the structure. The constitutive relationship between stress and strain is the generalized Hooke’s law.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…The governing equation for a continuum undergoing motion is given by Cauchy’s equation in three dimensions60, 61: ρνit=·σij+fi where the subscript i is a free index as before, f i is the external force, and v i is the velocity of the structure. The constitutive relationship between stress and strain is the generalized Hooke’s law.…”
Section: Methodsmentioning
confidence: 99%
“…Thus the information about mesh deformation, velocity and the fluid pressure is exchanged through this interface. The construction of the FSI method is implemented by coupling a computational fluid dynamics (CFD) solver27 with a computational structural dynamics (CSD) solver60, 61. The two component solvers can be substituted with any other similar-functioned CFD and CSD solvers for various FSI phenomena.…”
Section: Methodsmentioning
confidence: 99%
“…The existing finite volume paradigms discussed in the structural mechanics community can be classified into two families, depending on the localisation of the unknowns in the computational mesh: the cell-centred finite volume (CCFV) method [4,11,22,25] defines the unknowns at the centroid of the mesh elements, whereas the vertex-centred finite volume (VCFV) strategy [40,42,49] sets the unknowns at the mesh nodes. A major limitation of the CCFV method is the poor approximation of the gradient of the displacements at the faces using unstructured meshes [2,7].…”
Section: Introductionmentioning
confidence: 99%
“…In 2005, large strain hyperelastic problems were addressed by Bijelonja et al [27] using FV. In 2007, Xia et al [28] solved an elastic 3D problem using an implicit FVM scheme and Lv et al [29], based also on an implicit formulation and by adopting unstructured meshes, applied FV to both solid and fluid flow problems. In the same year, Limache and Idelsohn [30] emphasized that the FVM approach is a very interesting route for solving solid mechanics problems, indicating several positive factors.…”
Section: Developments Of the Method-historical Viewmentioning
confidence: 99%