Abstract

Variational multiscale methods, and their precursors, stabilized methods, have been playing a core-method role in semi-discrete and space–time (ST) flow computations for decades. These methods are sometimes supplemented with discontinuity-capturing (DC) methods. The stabilization and DC parameters embedded in most of these methods play a significant role. Various well-performing stabilization and DC parameters have been introduced in both the semi-discrete and ST contexts. The parameters almost always involve some element length expressions, most of the time in specific directions, such as the direction of the flow or solution gradient. Until recently, stabilization and DC parameters originally intended for finite element discretization were being used also for isogeometric discretization. Recently, element lengths and stabilization and DC parameters targeting isogeometric discretization were introduced for ST and semi-discrete computations, and these expressions are also applicable to finite element discretization. The key stages of deriving the direction-dependent element length expression were mapping the direction vector from the physical (ST or space-only) element to the parent element in the parametric space, accounting for the discretization spacing along each of the parametric coordinates, and mapping what has been obtained back to the physical element. Targeting B-spline meshes for complex geometries, we introduce here new element length expressions, which are outcome of a clear and convincing derivation and more suitable for element-level evaluation. The new expressions are based on a preferred parametric space and a transformation tensor that represents the relationship between the integration and preferred parametric spaces. The test computations we present for advection-dominated cases, including 2D computations with complex meshes, show that the proposed element length expressions result in good solution profiles.

Highlights

  • In this article we introduce directional element length expressions for B-spline meshes used in flow computations with the stabilized and variational multiscale (VMS) methods, discontinuity-capturing

  • The Arbitrary Lagrangian–Eulerian (ALE)-SUPS, residual-based VMS (RBVMS) and ALE-VMS have been applied to many classes of fluid–structure interaction (FSI), moving boundaries and interfaces (MBI) and fluid mechanics problems

  • It was shown that when the element length expression is based on the integration parametric space, the variation with the node numbering could be by a factor as high as 1.9 for 3D elements and 2.2 for ST elements

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Summary

Stabilized and VMS methods

Stabilized and VMS methods have for decades been playing a core-method role in flow analysis with semi-discrete and space–time (ST) computational methods. The incompressibleflow Streamline-Upwind/Petrov-Galerkin (SUPG) [1,2] and compressible-flow SUPG [3,4,5] methods are two of the earliest and most widely used stabilized methods. The incompressible-flow Pressure-Stabilizing/Petrov-Galerkin (PSPG) method [6,7], with its Stokes-flow version introduced in [8], is among the earliest and most widely used. These methods bring numerical stability in computation of flow problems at high Reynolds or Mach numbers and when using equal-order basis functions for velocity and pressure in incompressible flows. The residual-based VMS (RBVMS) [9,10,11,12], which is widely used, subsumes its precursor SUPG/PSPG

DC methods
Stabilized and VMS ST computational methods
ST Slip Interface method
ST Isogeometric Analysis
Stabilization parameters and element lengths
Directional element lengths for isogeometric discretization
Directional element lengths for B-spline elements
1.10 Outline of the remaining sections
Advection–diffusion equation
ST SUPG method
Element length
Element metric tensor in space
Formulating D for B-spline elements
RQD-EL
RQD-MIN
Extension to multiple dimensions
Scaling study in 1D
Advection skew to the mesh
Scaling
Stabilization parameter
DC parameter
Full Text
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