Abstract:Abstract. In this paper Fluid-structure interaction (FSI) simulations of artery aneurysms are carried out where both the fluid flow and the hyperelastic material are incompressible. We focus on time-dependent formulations adopting a monolithic approach, where the deformation of the fluid domain is taken into account according to an Arbitrary Lagrangian Eulerian (ALE) scheme. The exact Jacobian matrix is implemented by using automatic differentiation tools. The system is modeled using a specific equation shuffl… Show more
“…Two 2D geometries are considered, involving a venous valve and a brain aneurysm. The AS preconditioner has already been tested on these two geometries in Aulisa et al and Calandrini and Aulisa . A brief description of the function used in the venous valve simulations is also given.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Two 3D geometries are presented, a brain aneurysm and an aortic aneurysm. The AS preconditioner has already been tested on the 3D brain aneurysm geometry in Aulisa et al…”
Section: Numerical Resultsmentioning
confidence: 99%
“…To analyze the FS preconditioner for the level subsolvers, we compare its performance with the preconditioner in Aulisa et al, which is of pure domain decomposition type. In Aulisa et al and Calandrini et al, the Krylov solver in Aulisa et al has been applied to solve FSI problems with biomedical applications, namely, it has been used for stented cerebral aneurysm simulations in Aulisa et al and for magnetic drug targeting (MDT) procedures in Calandrini et al We intend to show that an FS approach is more suitable for biomedical FSI problems, where a Krylov solver preconditioned with a multigrid method is adopted.…”
Section: Introductionmentioning
confidence: 99%
“…In Richter, 44 GMG is used as a preconditioner for GMRES as we do, but for the smoothing strategy, a partitioned iteration is used based on the idea provided in van Brummelen et al 45 For an overview of some of the most popular methodologies to solve numerically the haemodynamic FSI systems, please refer to the introduction in Crosetto, 46 where a class of block triangular preconditioners is described, obtained by exploiting the block-structure of the FSI linear system.To analyze the FS preconditioner for the level subsolvers, we compare its performance with the preconditioner in Aulisa et al, 47 which is of pure domain decomposition type. In Aulisa et al 48,49 and Calandrini et al,50 the Krylov solver in Aulisa et al 47 has been applied to solve FSI problems with biomedical applications, namely, it has been used for stented cerebral aneurysm simulations in Aulisa et al 48,49 and for magnetic drug targeting (MDT) procedures in Calandrini et al 50 We intend to show that an FS approach is more suitable for biomedical FSI problems, where a Krylov solver preconditioned with a multigrid method is adopted.The biomedical applications considered for the tests include aneurysm and venous valve geometries. Both 2D and 3D simulations are carried out.…”
We present a novel preconditioning technique for Krylov subspace algorithms to solve fluid‐structure interaction (FSI) linearized systems arising from finite element discretizations. An outer Krylov subspace solver preconditioned with a geometric multigrid (GMG) algorithm is used, where for the multigrid level subsolvers, a field‐split (FS) preconditioner is proposed. The block structure of the FS preconditioner is derived using the physical variables as splitting strategy. To solve the subsystems originated by the FS preconditioning, an additive Schwarz (AS) block strategy is employed. The proposed FS preconditioner is tested on biomedical FSI applications. Both 2D and 3D simulations are carried out considering aneurysm and venous valve geometries. The performance of the FS preconditioner is compared with that of a second preconditioner of pure domain decomposition type.
“…Two 2D geometries are considered, involving a venous valve and a brain aneurysm. The AS preconditioner has already been tested on these two geometries in Aulisa et al and Calandrini and Aulisa . A brief description of the function used in the venous valve simulations is also given.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Two 3D geometries are presented, a brain aneurysm and an aortic aneurysm. The AS preconditioner has already been tested on the 3D brain aneurysm geometry in Aulisa et al…”
Section: Numerical Resultsmentioning
confidence: 99%
“…To analyze the FS preconditioner for the level subsolvers, we compare its performance with the preconditioner in Aulisa et al, which is of pure domain decomposition type. In Aulisa et al and Calandrini et al, the Krylov solver in Aulisa et al has been applied to solve FSI problems with biomedical applications, namely, it has been used for stented cerebral aneurysm simulations in Aulisa et al and for magnetic drug targeting (MDT) procedures in Calandrini et al We intend to show that an FS approach is more suitable for biomedical FSI problems, where a Krylov solver preconditioned with a multigrid method is adopted.…”
Section: Introductionmentioning
confidence: 99%
“…In Richter, 44 GMG is used as a preconditioner for GMRES as we do, but for the smoothing strategy, a partitioned iteration is used based on the idea provided in van Brummelen et al 45 For an overview of some of the most popular methodologies to solve numerically the haemodynamic FSI systems, please refer to the introduction in Crosetto, 46 where a class of block triangular preconditioners is described, obtained by exploiting the block-structure of the FSI linear system.To analyze the FS preconditioner for the level subsolvers, we compare its performance with the preconditioner in Aulisa et al, 47 which is of pure domain decomposition type. In Aulisa et al 48,49 and Calandrini et al,50 the Krylov solver in Aulisa et al 47 has been applied to solve FSI problems with biomedical applications, namely, it has been used for stented cerebral aneurysm simulations in Aulisa et al 48,49 and for magnetic drug targeting (MDT) procedures in Calandrini et al 50 We intend to show that an FS approach is more suitable for biomedical FSI problems, where a Krylov solver preconditioned with a multigrid method is adopted.The biomedical applications considered for the tests include aneurysm and venous valve geometries. Both 2D and 3D simulations are carried out.…”
We present a novel preconditioning technique for Krylov subspace algorithms to solve fluid‐structure interaction (FSI) linearized systems arising from finite element discretizations. An outer Krylov subspace solver preconditioned with a geometric multigrid (GMG) algorithm is used, where for the multigrid level subsolvers, a field‐split (FS) preconditioner is proposed. The block structure of the FS preconditioner is derived using the physical variables as splitting strategy. To solve the subsystems originated by the FS preconditioning, an additive Schwarz (AS) block strategy is employed. The proposed FS preconditioner is tested on biomedical FSI applications. Both 2D and 3D simulations are carried out considering aneurysm and venous valve geometries. The performance of the FS preconditioner is compared with that of a second preconditioner of pure domain decomposition type.
“…A validation of the FSI model and solver throughout a series of 2D and three‐dimensional (3D) benchmark tests can be found in Aulisa et al, where the results obtained were compared with several existing FSI models and solvers . Previous applications of our FSI model and solver to hemodynamics problems can be found in Aulisa et al and Calandrini et al Before discussing the formulation of the problem, we introduce some notations.…”
Venous valves are bicuspidal valves that ensure that blood in veins only flows back to the heart. To prevent retrograde blood flow, the two intraluminal leaflets meet in the center of the vein and occlude the vessel. In fluid-structure interaction (FSI) simulations of venous valves, the large structural displacements may lead to mesh deteriorations and entanglements, causing instabilities of the solver and, consequently, the numerical solution to diverge. In this paper, we propose an arbitrary Lagrangian-Eulerian (ALE) scheme for FSI simulations designed to solve these instabilities. A monolithic formulation for the FSI problem is considered, and due to the complexity of the operators, the exact Jacobian matrix is evaluated using automatic differentiation. The method relies on the introduction of a staggered in time velocity to improve stability, and on fictitious springs to model the contact force of the valve leaflets. Because the large structural displacements may compromise the quality of the fluid mesh as well, a smoother fluid displacement, obtained with the introduction of a scaling factor that measures the distance of a fluid element from the valve leaflet tip, guarantees that there are no mesh entanglements in the fluid domain. To further improve stability, a streamline upwind Petrov-Galerkin (SUPG) method is employed. The proposed ALE scheme is applied to a two-dimensional (2D) model of a venous valve. The presented simulations show that the proposed method deals well with the large structural displacements of the problem, allowing a reconstruction of the valve behavior in both the opening and closing phase.
We present fluid-structure interaction simulations of magnetic drug targeting (MDT) in blood flows. In this procedure, a drug is attached to ferromagnetic particles to externally direct it to a specific target after it is injected inside the body. The goal is to minimize the healthy tissue affected by the treatment and to maximize the number of particles that reach the target location. Magnetic drug targeting has been studied both experimentally and theoretically by several authors. In recent years, computational fluid dynamics simulations of MDT in blood flows have been conducted to obtain further insight on the combination of parameters that provide the best capture efficiency. However, to this day, no computational study addressed MDT in a fluid-structure interaction setting. With this paper, we aim to fill this gap and investigate the impact of the solid deformation on the capture efficiency.
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