2017
DOI: 10.1016/j.compfluid.2017.08.013
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A variationally bounded scheme for delayed detached eddy simulation: Application to vortex-induced vibration of offshore riser

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Cited by 31 publications
(31 citation statements)
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“…We observe more intense vortical structures near the location of large response amplitude. A more detailed analysis of the response amplitude and its relation to the trajectories along the riser can be found in [53]. This demonstration concludes that the present solver with common-refinement scheme is able to capture the physics as well as the response of the flexible riser reasonably well for non-matching unstructured meshes.…”
Section: Vortex Patternssupporting
confidence: 52%
“…We observe more intense vortical structures near the location of large response amplitude. A more detailed analysis of the response amplitude and its relation to the trajectories along the riser can be found in [53]. This demonstration concludes that the present solver with common-refinement scheme is able to capture the physics as well as the response of the flexible riser reasonably well for non-matching unstructured meshes.…”
Section: Vortex Patternssupporting
confidence: 52%
“…Compared to direct numerical simulation (DNS) and large eddy simulation (LES) methods, the delayed detached eddy simulation (DDES) method has significant advantages to save the computational resources while keeping the reasonable accuracy for the separated turbulent flow, as demonstrated by [44] for large-scale fluid-structure simulations. The DDES model offers an effective and reasonable way to simulate the vortex structures played during a flapping flight, hence we employ this model in our computational framework.…”
Section: Aspects Of Computational Modelingmentioning
confidence: 99%
“…Apart from the high density ratio between the two phases, ie, ρ=ρ1normalffalse/ρ2normalf=833.3, a low structure‐to‐fluid density ratio false(ρsfalse/ρ1normalf=0.5false) based on the denser fluid has been chosen. The initial condition for the order parameter is given as ϕfalse(x,y,0false)=tanh-1.5pt()y2ϵ. We have employed the hybrid RANS/LES model discussed in the work of Joshi and Jaiman for modeling the turbulent effects. The Reynolds number is defined based on the maximum velocity achieved by the cylinder and its diameter with respect to the denser fluid, ie, Re=ρ1normalfUcylDfalse/μ1normalf30,000.…”
Section: Numerical Testsmentioning
confidence: 99%