2011
DOI: 10.1016/j.compfluid.2011.03.015
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A high-order spectral difference method for unstructured dynamic grids

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Cited by 49 publications
(57 citation statements)
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“…The performance of the developed solver for low Mach number flow is first tested by computing the steady viscous flow over a NACA0012 airfoil at Re¼ 5000, Ma ∞ ¼ 0.05 and zero AOA with a 3rd order accurate SD scheme and an implicit LU-SGS time integration (Yu et al, 2011) on a coarse mesh. The residual convergence history, pressure coefficient (C P ) contour, and the Mach number contour are displayed in Fig.…”
Section: Resultsmentioning
confidence: 99%
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“…The performance of the developed solver for low Mach number flow is first tested by computing the steady viscous flow over a NACA0012 airfoil at Re¼ 5000, Ma ∞ ¼ 0.05 and zero AOA with a 3rd order accurate SD scheme and an implicit LU-SGS time integration (Yu et al, 2011) on a coarse mesh. The residual convergence history, pressure coefficient (C P ) contour, and the Mach number contour are displayed in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…2. Grid deformation strategy associated with the kinematics of the airfoil can be found in the paper by Yu et al (2011). The aerodynamic parameters are specified as follows.…”
Section: Simulation Parametersmentioning
confidence: 99%
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“…Mohammad et al [32] carried out LES of flow past a cylinder, Parsani et al [34] studied flow induced noise, Lodato et al [28] did wall modeled LES, Ou et al [33] and Yu et al [49] applied the SD method to moving grids, to name just a few. As pointed out by Bassi and Rebay [1,2], for high-order methods involving curved boundaries, the use of high-order elements is crucial for achieving smooth solution and for improving robustness, examples for the SD method can be found in [22,24].…”
Section: The Sd Methodsmentioning
confidence: 99%