MESOSCALE SIMULATIONS OF POWDER COMPACTION

Author(s):  
Ilya. Lomov ◽  
Don Fujino ◽  
Tarabay Antoun ◽  
Benjamin Liu ◽  
Mark Elert ◽  
...  
2018 ◽  
Vol 12 (1) ◽  
pp. JAMDSM0022-JAMDSM0022 ◽  
Author(s):  
Yu LEI ◽  
Shiwei YAN ◽  
Shangyu HUANG ◽  
Wei LIU ◽  
Shiming SUN ◽  
...  

2010 ◽  
Vol 99 (10) ◽  
pp. 4307-4316 ◽  
Author(s):  
Xiaoping Cao ◽  
Mikayla Morganti ◽  
Bruno C. Hancock ◽  
Victoria M. Masterson

2015 ◽  
Vol 35 (2) ◽  
pp. 525-531 ◽  
Author(s):  
K. Rubešová ◽  
T. Hlásek ◽  
V. Jakeš ◽  
Š. Huber ◽  
J. Hejtmánek ◽  
...  

Author(s):  
Timothy W. Juliano ◽  
Branko Kosović ◽  
Pedro A. Jiménez ◽  
Masih Eghdami ◽  
Sue Ellen Haupt ◽  
...  

AbstractGenerating accurate weather forecasts of planetary boundary layer (PBL) properties is challenging in many geographical regions, oftentimes due to complex topography or horizontal variability in, for example, land characteristics. While recent advances in high-performance computing platforms have led to an increase in the spatial resolution of numerical weather prediction (NWP) models, the horizontal grid cell spacing (Δ x) of many regional-scale NWP models currently fall within or are beginning to approach the gray zone (i.e., Δ x ≈ 100 – 1000 m). At these grid cell spacings, three-dimensional (3D) effects are important, as the most energetic turbulent eddies are neither fully parameterized (as in traditional mesoscale simulations) nor fully resolved [as in traditional large eddy simulations (LES)]. In light of this modeling challenge, we have implemented a 3D PBL parameterization for high-resolution mesoscale simulations using the Weather Research and Forecasting model. The PBL scheme, which is based on the algebraic model developed by Mellor and Yamada, accounts for the 3D effects of turbulence by calculating explicitly the momentum, heat, and moisture flux divergences in addition to the turbulent kinetic energy. In this study, we present results from idealized simulations in the gray zone that illustrate the benefit of using a fully consistent turbulence closure framework under convective conditions. While the 3D PBL scheme reproduces the evolution of convective features more appropriately than the traditional 1D PBL scheme, we highlight the need to improve the turbulent length scale formulation.


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