2018
DOI: 10.1016/j.jcp.2018.03.028
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A family of position- and orientation-independent embedded boundary methods for viscous flow and fluid–structure interaction problems

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Cited by 29 publications
(31 citation statements)
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“…Cottet and Maitre 34 Continuous forcing IBM FDM Diffused momentum forcing Huang and Sung 32 Yu 35 Fictitious domain method Zhang et al 33 FVM Fedkiw 36 Discrete forcing IBM FDM Ghost-fluid interpolation Liu et al 30 FEM Ghost-cell interpolation Mittal et al 31 FDM Degroote et al 37 Quasi-Newton method Li et al 38 Continuous Robin boundary condition Wang et al 27 EBM FVM Fluid-solid Riemann problem Huang et al 28 FIVER Li and Lai 26 IIM FDM Second-order projection method Present work FVM Level set function-based direct application of BCs at interface limited by the difficulty in solving highly nonlinear algebraic system, 24 and ALE methods are limited by the need to remesh and difficulty in handling large deformation. 19 The mesh motion problem observed in ALE is resolved in HLE method using a fixed Eulerian mesh in the fluid, with a special treatment for the cells near the solid-fluid interface.…”
Section: Reference Hle Methods Discretisation Methods Implementation Ofmentioning
confidence: 99%
“…Cottet and Maitre 34 Continuous forcing IBM FDM Diffused momentum forcing Huang and Sung 32 Yu 35 Fictitious domain method Zhang et al 33 FVM Fedkiw 36 Discrete forcing IBM FDM Ghost-fluid interpolation Liu et al 30 FEM Ghost-cell interpolation Mittal et al 31 FDM Degroote et al 37 Quasi-Newton method Li et al 38 Continuous Robin boundary condition Wang et al 27 EBM FVM Fluid-solid Riemann problem Huang et al 28 FIVER Li and Lai 26 IIM FDM Second-order projection method Present work FVM Level set function-based direct application of BCs at interface limited by the difficulty in solving highly nonlinear algebraic system, 24 and ALE methods are limited by the need to remesh and difficulty in handling large deformation. 19 The mesh motion problem observed in ALE is resolved in HLE method using a fixed Eulerian mesh in the fluid, with a special treatment for the cells near the solid-fluid interface.…”
Section: Reference Hle Methods Discretisation Methods Implementation Ofmentioning
confidence: 99%
“…To this end, the Eulerian framework of the AERO Suite of codes 42,43 developed at Stanford University for the simulation of highly nonlinear FSI phenomena with topological changes is chosen to perform the FSI simulations of parachute inflation dynamics (PID) reported herein. This computational framework is equipped with the FIVER (finite volume method with exact two-phase Riemann problems) embedded boundary method for FSI, 8,[44][45][46][47] which has been extensively verified and validated for complex multimaterial problems. 9,10,48 Specifically, all FSI computations reported in this section are performed using the SA turbulence model implemented in conservation form in AERO Suite's massively parallel flow solver AERO-F.…”
Section: Computational Frameworkmentioning
confidence: 99%
“…In addition, there are several more powerful nonlinear aeroelastic computer codes on the subject of computational aeroelasticity with high fidelity models and fluid structure interaction with reduced order models (ROMs) such as ARMA-ROM, Volterra-ROM, and POD-ROM. Many important works on this subject were done by Farhat et al [23][24][25][26] at Stanford University (Mech and Aerospace Engr Dept). A linearized synchronous and staggered fluid-structure time-integration interaction algorithms [27][28][29] were introduced and applied to predict the transient aeroelastic response of a reduced-order model of a complete F-16 aircraft configuration at a given Mach number.…”
Section: Introductionmentioning
confidence: 99%