2015
DOI: 10.1016/j.procs.2015.05.228
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Coupling Navier-stokes and Cahn-hilliard Equations in a Two-dimensional Annular flow Configuration

Abstract: In this work, we present a novel isogeometric analysis discretization for the Navier-StokesCahn-Hilliard equation, which uses divergence-conforming spaces. Basis functions generated with this method can have higher-order continuity, and allow to directly discretize the higherorder operators present in the equation. The discretization is implemented in PetIGA-MF, a high-performance framework for discrete differential forms. We present solutions in a twodimensional annulus, and model spinodal decomposition under… Show more

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Cited by 21 publications
(15 citation statements)
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“…The temporal integration schemes are applied to the variational formulation presented in equations (55)- (56). The fully discrete formulations for the provably-stable methods to solve the phase-field crystal equation can be defined as: given φ…”
Section: Phase-field Crystal Equationmentioning
confidence: 99%
See 1 more Smart Citation
“…The temporal integration schemes are applied to the variational formulation presented in equations (55)- (56). The fully discrete formulations for the provably-stable methods to solve the phase-field crystal equation can be defined as: given φ…”
Section: Phase-field Crystal Equationmentioning
confidence: 99%
“…The method has successfully been applied in its Galerkin version to solve the Cahn-Hilliard equation [21,23], the advective [39] and Navier-Stokes-CahnHilliard equations [19,56], the Swift-Hohenberg equation [24] and the phasefield crystal equation [25,54,57]. IGA possesses some advantages over standard finite element methods, which include being able to easily generate high-order, globally continuous basis functions as well as exact geometrical representations as the finite element space is refined.…”
Section: Introductionmentioning
confidence: 99%
“…The strategy was implemented in PetIGA-MF [18], a toolbox built on top of PetIGA [19] extending it to support flexible and parallel multi-field discretizations based on structure-preserving B-spline spaces, in the sense of [2]. For examples of the Navier-Stokes-Cahn-Hilliard model using PetIGA-MF see [44,45] . 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 As benchmark problems, we use the flows on a square and a cubic cavity, the flow in an eccentric annulus, and the flow in a hollow torus of eccentric annular cross-section.…”
Section: Performance Resultsmentioning
confidence: 99%
“…On the middle pair of elements, the two basis functions that are discontinuous at x M are shown in black. The positions of the nodes are determined by d 1 and d 2 and, together with the asymptotic weights ω A 1 and ω A 2 , are computed from the (4 × 4) asymptotic system (29). The middle weight is computed from (30), which corresponds to the exactness of the rule when applied on the middle discontinuous basis function D M .…”
Section: Numerical Examples Of Derived Gaussian Rulesmentioning
confidence: 99%
“…Numerical integration is a fundamental ingredient of isogeometric analysis (IGA) and finite elements (FE), and its computational efficiency is essential. When simulating physical processes, e.g., [9,10,15,17,29], with Galerkin isogeometric discretizations, specific spline spaces appear when building mass and stiffness matrices. By construction, these spline spaces are of even degrees and the quadrature rules used to numerically integrate functions from these spaces are sub-optimal [2,5,16,26].…”
Section: Introductionmentioning
confidence: 99%