2020
DOI: 10.1007/978-3-030-39647-3_26
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Dynamical Degree Adaptivity for DG-LES Models

Abstract: Discontinuous Galerkin spatial discretizations of compressible flows allow to perform local degree adaptation (shortly, p-adaptation) in a very straightforward way and almost without computational overhead, as shown e.g. in [6]. Dynamical adaptation was also applied successfully to inviscid geophysical flows in [11, 12]. All the previous works relied however on a refinement criterion which essentially estimates the L 2 norm approximation error. In [10], we have argued that such a criterion may not be optimal f… Show more

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Cited by 2 publications
(3 citation statements)
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“…The maximum radial velocity chosen is v θmax = 0.5 and the vortex radius is R v = 0.41. The simple, undisturbed advection of this vortex was tested successfully for the resolutions employed here in [40,85]. A reference simulation without vortex was used to calibrate the introduction time, so as to allow the vortex to reach the cylinder at the instant of maximum lift.…”
Section: Interaction Of Vortex and Square Section Cylindermentioning
confidence: 99%
“…The maximum radial velocity chosen is v θmax = 0.5 and the vortex radius is R v = 0.41. The simple, undisturbed advection of this vortex was tested successfully for the resolutions employed here in [40,85]. A reference simulation without vortex was used to calibrate the introduction time, so as to allow the vortex to reach the cylinder at the instant of maximum lift.…”
Section: Interaction Of Vortex and Square Section Cylindermentioning
confidence: 99%
“…A vortex, with axis parallel to the wing and rotating in the counterclockwise direction, has been introduced in the developed velocity field obtained by the simulation of the flow around the SD7003 airfoil described in the previous subsection, in order to simulate the BVI phenomenon. The definition of the vortex is the one used by [15,24] inducing the velocity and pressure…”
Section: Simulation Of Parallel Bvimentioning
confidence: 99%
“…In [31,33] simple advection of this vortex was tested. The maximum radial velocity chosen is v θmax = 0.5 and the vortex radius is R v = 0.41.…”
Section: Interaction Of Vortex and Square Section Cylindermentioning
confidence: 99%