2016
DOI: 10.1016/j.jcp.2016.06.031
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An overset mesh approach for 3D mixed element high-order discretizations

Abstract: A parallel high-order Discontinuous Galerkin (DG) method is used to solve the compressible Navier-Stokes equations in an overset mesh framework. The DG solver has many capabilities including: hp-adaption, curved cells, support for hybrid, mixed-element meshes, and moving meshes. Combining these capabilities with overset grids allows the DG solver to be used in problems with bodies in relative motion and in a near-body offbody solver strategy. The overset implementation is constructed to preserve the design acc… Show more

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Cited by 67 publications
(12 citation statements)
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“…3 The overset grid method was first used in finite-difference structured CFD codes back in 1980s, 1 the 1990s saw the first implementations for structured-grid finite volume codes for maritime applications. 4 Currently, unstructured-grid finite volume codes [5][6][7][8][9] and higher-order finite element codes 10 often have an overset grid capabilities. In the current work, the overset grid technique is studied for face-based unstructured-grid finite volume viscous-flow codes, particularly for incompressible hydrodynamic flows at high Reynolds numbers.…”
Section: Introductionmentioning
confidence: 99%
“…3 The overset grid method was first used in finite-difference structured CFD codes back in 1980s, 1 the 1990s saw the first implementations for structured-grid finite volume codes for maritime applications. 4 Currently, unstructured-grid finite volume codes [5][6][7][8][9] and higher-order finite element codes 10 often have an overset grid capabilities. In the current work, the overset grid technique is studied for face-based unstructured-grid finite volume viscous-flow codes, particularly for incompressible hydrodynamic flows at high Reynolds numbers.…”
Section: Introductionmentioning
confidence: 99%
“…Overset-grid methods are also included in commercial and research software packages such as Star-CCM [12], Overflow [13] and Overture [14]. Most of these implementations, however, are at most fourthorder accurate in space [9,11,15,16,17,18]. Sixth-order finite-difference based methods have been presented in [19,13], while sixthorder finite volume based schemes are available in elsA [20].…”
Section: Introductionmentioning
confidence: 99%
“…The use of a static linear basis for ROM in Ω A limits its predictive capabilities. It is pointed out that the interface mismatches are not unique to ROM/FOM coupling, but more general issues for finite-element [73] and finite-volume [74] methods, especially with non-matching grids (i.e., inconsistent orders of modeling accuracy)-for example, the coupling of low-and high-order CFD solvers (FOMs) may require-for example-an overset-mesh approach [21,75]. Though such methods can be effective in coupling of low-and high-order FOMs, it is not clear whether such methods can be applied directly to ROM and FOM coupling since ROM evolves on a reduced dimensional trajectory determined by the basis, while the FOM (either with low-or high-order numerical methods) solves the dynamical system on the full state space trajectory.…”
Section: Performancementioning
confidence: 99%