2012
DOI: 10.1016/j.jcp.2012.05.015
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A second-order virtual node algorithm for nearly incompressible linear elasticity in irregular domains

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Cited by 7 publications
(8 citation statements)
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“…However, most of these methods typically require tools not frequently available in standard finite element and finite difference software packages. Examples of such approaches include the extended and composite finite element methods (e.g., [31,12,23,13,32,55,7,4]), immersed interface methods (e.g., [40,43,60,44,65]), virtual node methods with embedded boundary conditions (e.g., [3,73,34]), matched interface and boundary methods (e.g., [71,68,69,67,72]), modified finite volume/embedded boundary/cut-cell methods/ghost-fluid methods (e.g., [27,36,19,25,26,35,47,70,48,37,46,64,49,9,10,52,53,33,63]). In another approach, known as the fictitious domain method (e.g., [28,29,56,45]), the original system is either augmented with equations for Lagrange multipliers to enforce the boundary conditions, or the penalty method is used to enforce the boundary condi-tions weakly.…”
Section: Introductionmentioning
confidence: 99%
“…However, most of these methods typically require tools not frequently available in standard finite element and finite difference software packages. Examples of such approaches include the extended and composite finite element methods (e.g., [31,12,23,13,32,55,7,4]), immersed interface methods (e.g., [40,43,60,44,65]), virtual node methods with embedded boundary conditions (e.g., [3,73,34]), matched interface and boundary methods (e.g., [71,68,69,67,72]), modified finite volume/embedded boundary/cut-cell methods/ghost-fluid methods (e.g., [27,36,19,25,26,35,47,70,48,37,46,64,49,9,10,52,53,33,63]). In another approach, known as the fictitious domain method (e.g., [28,29,56,45]), the original system is either augmented with equations for Lagrange multipliers to enforce the boundary conditions, or the penalty method is used to enforce the boundary condi-tions weakly.…”
Section: Introductionmentioning
confidence: 99%
“…Explicit boundary discretizations, such as embedded surface meshes, show their unique merits in modeling the sub-cell geometry and enforcing precise boundary conditions [Azevedo et al 2016;Schroeder et al 2012]. These embedded discretizations of the variational type, are focused on handling Dirichlet boundaries Zhu et al 2012], which inspired our discretization for solving steady-state flow problems. These discretizations can conveniently accommodate adaptive resolution [Ando et al 2013] and flows in containers with deforming geometry [Feldman et al 2005].…”
Section: Related Workmentioning
confidence: 99%
“…Our model: quasi-incompressible Stokes. The aforementioned relation of Stokes and linear elasticity has previously been leveraged primarily to develop discretization and solution schemes for incompressible or near-incompressible elasticity that draw inspiration from established methods for Stokes [Gaspar et al 2008;Zhu et al 2012]. However, directly pursuing a discretization of the Stokes problem has its own subtleties; due to the incompressibility constraint, the associated discretizations -and especially variational formulations -take the form of saddle point problems, restricting somewhat the options for associated numerical solvers.…”
Section: Governing Partial Differential Equationsmentioning
confidence: 99%
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“…They generate an explicit discontinuity-aligned boundary mesh and compute surface integrals using the divergence-theorem. VNA-based approaches following the same strategy were also developed in the engineering community [Bedrossian et al 2010;Zhu et al 2012]. Over the years several approaches based on equivalent polynomials [Ventura 2006], adaptive quadrature [Müller et al 2012] or variable quadrature weights [Holdych et al 2008] were developed.…”
Section: Related Workmentioning
confidence: 99%