Frontiers in Digital Humanities | |
What is the smallest physically acceptable scale for 1D turbulence schemes? | |
Honnert, Rachel2  ry6  Masson, Valé8  | |
[1] AtmosphèCentre National de Recherches MéEtudes de l'o France/CNRS, Toulouse, France;orologique, Méorologiques, Groupe d're Mété | |
关键词: boundary-layer meteorology; Turbulence; parametrization; gray zone; large-Eddy Simulations; | |
DOI : 10.3389/feart.2014.00027 | |
学科分类:社会科学、人文和艺术(综合) | |
来源: Frontiers | |
【 摘 要 】
In numerical weather prediction (NWP) models, at mesoscale, the subgrid convective boundary-layer turbulence is dominated by the uni-directional (1D) vertical thermal production. In Large-Eddy Simulations (LES), the thermal plumes are resolved and the residual subgrid turbulent motions are homogeneous and isotropic, thus three-dimensional (3D), resulting from the dynamical production. This article sets the critical horizontal resolution for which the usually 1D turbulence schemes of NWP models must be replaced by 3D turbulence schemes. LES from five dry and cumulus-topped free convective boundary layers and one forced convective boundary layer are performed. From these LES data, the thermal production and vertical and horizontal dynamical productions are calculated at several resolutions from LES to mesoscale. It appears that the production terms of both dry and cumulus-topped free convective boundary layers have the same behavior. A pattern emerges whenever data are ranked by the resolution scaled by the size of thermal plumes, (h + hc , where h is the boundary-layer height and hc is the depth of the cloud layer). In free onvective boundary layers, the critical horizontal resolution for which the horizontal motions must be represented is 0.5(h + hc ). However, the critical horizontal resolution in the forced convective boundary layer case is 3(h + hc ).
【 授权许可】
CC BY
【 预 览 】
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RO201904022929413ZK.pdf | 872KB | download |