|
|
|
|
| LEADER |
01000caa a22002652 4500 |
| 001 |
NLM357167546 |
| 003 |
DE-627 |
| 005 |
20240902232504.0 |
| 007 |
cr uuu---uuuuu |
| 008 |
231226s2023 xx |||||o 00| ||eng c |
| 024 |
7 |
|
|a 10.1016/j.jcp.2023.112174
|2 doi
|
| 028 |
5 |
2 |
|a pubmed24n1520.xml
|
| 035 |
|
|
|a (DE-627)NLM357167546
|
| 035 |
|
|
|a (NLM)37214277
|
| 035 |
|
|
|a (PII)112174
|
| 040 |
|
|
|a DE-627
|b ger
|c DE-627
|e rakwb
|
| 041 |
|
|
|a eng
|
| 100 |
1 |
|
|a Kolahdouz, Ebrahim M
|e verfasserin
|4 aut
|
| 245 |
1 |
2 |
|a A sharp interface Lagrangian-Eulerian method for flexible-body fluid-structure interaction
|
| 264 |
|
1 |
|c 2023
|
| 336 |
|
|
|a Text
|b txt
|2 rdacontent
|
| 337 |
|
|
|a ƒaComputermedien
|b c
|2 rdamedia
|
| 338 |
|
|
|a ƒa Online-Ressource
|b cr
|2 rdacarrier
|
| 500 |
|
|
|a Date Revised 02.09.2024
|
| 500 |
|
|
|a published: Print-Electronic
|
| 500 |
|
|
|a Citation Status PubMed-not-MEDLINE
|
| 520 |
|
|
|a This paper introduces a sharp-interface approach to simulating fluid-structure interaction (FSI) involving flexible bodies described by general nonlinear material models and across a broad range of mass density ratios. This new flexible-body immersed Lagrangian-Eulerian (ILE) scheme extends our prior work on integrating partitioned and immersed approaches to rigid-body FSI. Our numerical approach incorporates the geometrical and domain solution flexibility of the immersed boundary (IB) method with an accuracy comparable to body-fitted approaches that sharply resolve flows and stresses up to the fluid-structure interface. Unlike many IB methods, our ILE formulation uses distinct momentum equations for the fluid and solid subregions with a Dirichlet-Neumann coupling strategy that connects fluid and solid subproblems through simple interface conditions. As in earlier work, we use approximate Lagrange multiplier forces to treat the kinematic interface conditions along the fluid-structure interface. This penalty approach simplifies the linear solvers needed by our formulation by introducing two representations of the fluid-structure interface, one that moves with the fluid and another that moves with the structure, that are connected by stiff springs. This approach also enables the use of multi-rate time stepping, which allows us to use different time step sizes for the fluid and structure subproblems. Our fluid solver relies on an immersed interface method (IIM) for discrete surfaces to impose stress jump conditions along complex interfaces while enabling the use of fast structured-grid solvers for the incompressible Navier-Stokes equations. The dynamics of the volumetric structural mesh are determined using a standard finite element approach to large-deformation nonlinear elasticity via a nearly incompressible solid mechanics formulation. This formulation also readily accommodates compressible structures with a constant total volume, and it can handle fully compressible solid structures for cases in which at least part of the solid boundary does not contact the incompressible fluid. Selected grid convergence studies demonstrate second-order convergence in volume conservation and in the pointwise discrepancies between corresponding positions of the two interface representations as well as between first and second-order convergence in the structural displacements. The time stepping scheme is also demonstrated to yield second-order convergence. To assess and validate the robustness and accuracy of the new algorithm, comparisons are made with computational and experimental FSI benchmarks. Test cases include both smooth and sharp geometries in various flow conditions. We also demonstrate the capabilities of this methodology by applying it to model the transport and capture of a geometrically realistic, deformable blood clot in an inferior vena cava filter
|
| 650 |
|
4 |
|a Journal Article
|
| 650 |
|
4 |
|a Fluid-structure interaction
|
| 650 |
|
4 |
|a immersed Lagrangian-Eulerian method
|
| 650 |
|
4 |
|a immersed interface method
|
| 650 |
|
4 |
|a inferior vena cava filter
|
| 650 |
|
4 |
|a nonlinear continuum mechanics
|
| 700 |
1 |
|
|a Wells, David R
|e verfasserin
|4 aut
|
| 700 |
1 |
|
|a Rossi, Simone
|e verfasserin
|4 aut
|
| 700 |
1 |
|
|a Aycock, Kenneth I
|e verfasserin
|4 aut
|
| 700 |
1 |
|
|a Craven, Brent A
|e verfasserin
|4 aut
|
| 700 |
1 |
|
|a Griffith, Boyce E
|e verfasserin
|4 aut
|
| 773 |
0 |
8 |
|i Enthalten in
|t Journal of computational physics
|d 1986
|g 488(2023) vom: 01. Sept.
|w (DE-627)NLM098188844
|x 0021-9991
|7 nnns
|
| 773 |
1 |
8 |
|g volume:488
|g year:2023
|g day:01
|g month:09
|
| 856 |
4 |
0 |
|u http://dx.doi.org/10.1016/j.jcp.2023.112174
|3 Volltext
|
| 912 |
|
|
|a GBV_USEFLAG_A
|
| 912 |
|
|
|a SYSFLAG_A
|
| 912 |
|
|
|a GBV_NLM
|
| 912 |
|
|
|a GBV_ILN_350
|
| 951 |
|
|
|a AR
|
| 952 |
|
|
|d 488
|j 2023
|b 01
|c 09
|