Computation of moving boundaries and interfaces and stabilization parameters

By Tayfun E. Tezduyar. 2003

501 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/24f12c328f8316d4a887ce605fa3b3d49f2f0dc1

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In Computational Mechanics

Citations in the corpus

Topology optimisation for natural convection problems (2014, unknown): “o the full stabilisation parameters based on element matrices and vectors which has been simpliﬁed based on the assumption of using a single integration point to evaluate the stabilisation parameters [64]. All norms in this section are deﬁned to be the 2-norm. Likewise, for the thermal SUPG stabilis”
A coupled PFEM–Eulerian approach for the solution of porous FSI problems (2012, background): “We also note that it was proposed in [36] that the element lengths used in the second term (diffusive term) and third term (advective term) should be different, one being the diffusive element length and the other one being the advective element length.”
Isogeometric fluid-structure interaction: theory, algorithms, and computations (2008, unknown): “We focus on ALE and space-time methods (see, e.g., [31, 34, 39, 62, 63, 65 ]).”
Calculation of the advective limit of the SUPG stabilization parameter for linear and higher-order elements (2004, methodology): “UGN/RGN-based stabilization parameters In this subsection, we describe the versions of the stabilization parameters (ss) denoted by the subscript UGN, namely the ‘‘UGN/RGN-based’’ stabilization parameters [15,16].”
Variational multiscale residual-based turbulence modeling for large eddy simulation of incompressible flows (2007, unknown): “[12,67,72,39,66,14,3]).”
Finite elements in fluids: Stabilized formulations and moving boundaries and interfaces (2007, methodology): “Recognizing this second element length as a diffusion length scale, new stabilization parameters for the diffusive limit were introduced in [20,22,23,18].”
Improving stability of stabilized and multiscale formulations in flow simulations at small time steps (2010, unknown): “In the sequel we first provide the conventional definitions of the stabilization parameter τ appearing in (6), followed by the EVB definition, first proposed in [1, 2].”
Interface projection techniques for fluid–structure interaction modeling with moving-mesh methods (2008, methodology): “The version of the DSD/SST formulation given in [ 39 ] is clearer in representing the implementation used in the computations the T� AFSM has been practicing from the beginning (see Remark 1 in [40]).”
Isogeometric Fluid–structure Interaction Analysis with Applications to Arterial Blood Flow (2006, methodology): “Some of the other techniques include the coupled momentum method [14], the immersed finite element method [54], and the space-time finite element method [40] [41] [42].”
Diffuse-interface simulations of drop coalescence and retraction in viscoelastic fluids (2005, background): “The last stage of coalescence y a short-range molecular force in the model that is comparable to van der Waals force.”
Interface-tracking and interface-capturing techniques for finite element computation of moving boundaries and interfaces (2006, methodology): “For ways of calculating sSUPG, sPSPG and mLSIC, see [10,11,4].”
Numerical-performance studies for the stabilized space–time computation of wind-turbine rotor aerodynamics (2011, methodology): “The DSD/SST formulation was introduced in [4–6], was supplemented in [ 7 ] with advanced stabilization parameters, gained in [8] new versions with increased scope and robustness, and was elevated in [9] to a new version with an advanced turbulence model.”
Space-time finite element techniques for computation of fluid-structure interactions (2005, methodology): “For ways of calculating sSUPG, sPSPG and mLSIC, see [31,32,24].”