Vertically nested les for high-resolution simulation of the surface layer in PALM (version 5.0)

Research output: Contribution to journalArticleResearchpeer review

Authors

  • Sadiq Huq
  • Frederik De Roo
  • Siegfried Raasch
  • Matthias Mauder

External Research Organisations

  • Karlsruhe Institute of Technology (KIT)
  • Meteorologisk Institutt (MET)
View graph of relations

Details

Original languageEnglish
Pages (from-to)2523-2538
Number of pages16
JournalGeoscientific model development
Volume12
Issue number6
Early online date28 Jun 2019
Publication statusE-pub ahead of print - 28 Jun 2019

Abstract

Large-eddy simulation (LES) has become a well-established tool in the atmospheric boundary layer research community to study turbulence. It allows three-dimensional realizations of the turbulent fields, which large-scale models and most experimental studies cannot yield. To resolve the largest eddies in the mixed layer, a moderate grid resolution in the range of 10 to 100 m is often sufficient, and these simulations can be run on a computing cluster with a few hundred processors or even on a workstation for simple configurations. The desired resolution is usually limited by the computational resources. However, to compare with tower measurements of turbulence and exchange fluxes in the surface layer, a much higher resolution is required. In spite of the growth in computational power, a high-resolution LES of the surface layer is often not feasible: to fully resolve the energy-containing eddies near the surface, a grid spacing of O(1 m) is required. One way to tackle this problem is to employ a vertical grid nesting technique, in which the surface is simulated at the necessary fine grid resolution, and it is coupled with a standard, coarse, LES that resolves the turbulence in the whole boundary layer. We modified the LES model PALM (Parallelized Large-eddy simulation Model) and implemented a two-way nesting technique, with coupling in both directions between the coarse and the fine grid. The coupling algorithm has to ensure correct boundary conditions for the fine grid. Our nesting algorithm is realized by modifying the standard third-order Runge-Kutta time stepping to allow communication of data between the two grids. The two grids are concurrently advanced in time while ensuring that the sum of resolved and sub-grid-scale kinetic energy is conserved. We design a validation test and show that the temporally averaged profiles from the fine grid agree well compared to the reference simulation with high resolution in the entire domain. The overall performance and scalability of the nesting algorithm is found to be satisfactory. Our nesting results in more than 80 % savings in computational power for 5 times higher resolution in each direction in the surface layer.

ASJC Scopus subject areas

Cite this

Vertically nested les for high-resolution simulation of the surface layer in PALM (version 5.0). / Huq, Sadiq; De Roo, Frederik; Raasch, Siegfried et al.
In: Geoscientific model development, Vol. 12, No. 6, 28.06.2019, p. 2523-2538.

Research output: Contribution to journalArticleResearchpeer review

Huq S, De Roo F, Raasch S, Mauder M. Vertically nested les for high-resolution simulation of the surface layer in PALM (version 5.0). Geoscientific model development. 2019 Jun 28;12(6):2523-2538. Epub 2019 Jun 28. doi: 10.5194/gmd-12-2523-2019, 10.15488/5052
Huq, Sadiq ; De Roo, Frederik ; Raasch, Siegfried et al. / Vertically nested les for high-resolution simulation of the surface layer in PALM (version 5.0). In: Geoscientific model development. 2019 ; Vol. 12, No. 6. pp. 2523-2538.
Download
@article{a67e63aceac7419f8e48b2f83e094d89,
title = "Vertically nested les for high-resolution simulation of the surface layer in PALM (version 5.0)",
abstract = "Large-eddy simulation (LES) has become a well-established tool in the atmospheric boundary layer research community to study turbulence. It allows three-dimensional realizations of the turbulent fields, which large-scale models and most experimental studies cannot yield. To resolve the largest eddies in the mixed layer, a moderate grid resolution in the range of 10 to 100 m is often sufficient, and these simulations can be run on a computing cluster with a few hundred processors or even on a workstation for simple configurations. The desired resolution is usually limited by the computational resources. However, to compare with tower measurements of turbulence and exchange fluxes in the surface layer, a much higher resolution is required. In spite of the growth in computational power, a high-resolution LES of the surface layer is often not feasible: to fully resolve the energy-containing eddies near the surface, a grid spacing of O(1 m) is required. One way to tackle this problem is to employ a vertical grid nesting technique, in which the surface is simulated at the necessary fine grid resolution, and it is coupled with a standard, coarse, LES that resolves the turbulence in the whole boundary layer. We modified the LES model PALM (Parallelized Large-eddy simulation Model) and implemented a two-way nesting technique, with coupling in both directions between the coarse and the fine grid. The coupling algorithm has to ensure correct boundary conditions for the fine grid. Our nesting algorithm is realized by modifying the standard third-order Runge-Kutta time stepping to allow communication of data between the two grids. The two grids are concurrently advanced in time while ensuring that the sum of resolved and sub-grid-scale kinetic energy is conserved. We design a validation test and show that the temporally averaged profiles from the fine grid agree well compared to the reference simulation with high resolution in the entire domain. The overall performance and scalability of the nesting algorithm is found to be satisfactory. Our nesting results in more than 80 % savings in computational power for 5 times higher resolution in each direction in the surface layer.",
author = "Sadiq Huq and {De Roo}, Frederik and Siegfried Raasch and Matthias Mauder",
note = "Funding information: Author contributions. SH was the main developer of the model code, with FDR as side developer, SR supporting the code development and MM, SR and FDR supervising the development. The experiment was designed by SH, FDR, SR and MM and carried out by SH, who also performed the validation. Visualization was done by SH and the original draft written by SH and FDR, with review and editing by SR and MM. MM was responsible for funding acquisition and administration.",
year = "2019",
month = jun,
day = "28",
doi = "10.5194/gmd-12-2523-2019",
language = "English",
volume = "12",
pages = "2523--2538",
journal = "Geoscientific model development",
issn = "1991-959X",
publisher = "Copernicus Gesellschaft mbH",
number = "6",

}

Download

TY - JOUR

T1 - Vertically nested les for high-resolution simulation of the surface layer in PALM (version 5.0)

AU - Huq, Sadiq

AU - De Roo, Frederik

AU - Raasch, Siegfried

AU - Mauder, Matthias

N1 - Funding information: Author contributions. SH was the main developer of the model code, with FDR as side developer, SR supporting the code development and MM, SR and FDR supervising the development. The experiment was designed by SH, FDR, SR and MM and carried out by SH, who also performed the validation. Visualization was done by SH and the original draft written by SH and FDR, with review and editing by SR and MM. MM was responsible for funding acquisition and administration.

PY - 2019/6/28

Y1 - 2019/6/28

N2 - Large-eddy simulation (LES) has become a well-established tool in the atmospheric boundary layer research community to study turbulence. It allows three-dimensional realizations of the turbulent fields, which large-scale models and most experimental studies cannot yield. To resolve the largest eddies in the mixed layer, a moderate grid resolution in the range of 10 to 100 m is often sufficient, and these simulations can be run on a computing cluster with a few hundred processors or even on a workstation for simple configurations. The desired resolution is usually limited by the computational resources. However, to compare with tower measurements of turbulence and exchange fluxes in the surface layer, a much higher resolution is required. In spite of the growth in computational power, a high-resolution LES of the surface layer is often not feasible: to fully resolve the energy-containing eddies near the surface, a grid spacing of O(1 m) is required. One way to tackle this problem is to employ a vertical grid nesting technique, in which the surface is simulated at the necessary fine grid resolution, and it is coupled with a standard, coarse, LES that resolves the turbulence in the whole boundary layer. We modified the LES model PALM (Parallelized Large-eddy simulation Model) and implemented a two-way nesting technique, with coupling in both directions between the coarse and the fine grid. The coupling algorithm has to ensure correct boundary conditions for the fine grid. Our nesting algorithm is realized by modifying the standard third-order Runge-Kutta time stepping to allow communication of data between the two grids. The two grids are concurrently advanced in time while ensuring that the sum of resolved and sub-grid-scale kinetic energy is conserved. We design a validation test and show that the temporally averaged profiles from the fine grid agree well compared to the reference simulation with high resolution in the entire domain. The overall performance and scalability of the nesting algorithm is found to be satisfactory. Our nesting results in more than 80 % savings in computational power for 5 times higher resolution in each direction in the surface layer.

AB - Large-eddy simulation (LES) has become a well-established tool in the atmospheric boundary layer research community to study turbulence. It allows three-dimensional realizations of the turbulent fields, which large-scale models and most experimental studies cannot yield. To resolve the largest eddies in the mixed layer, a moderate grid resolution in the range of 10 to 100 m is often sufficient, and these simulations can be run on a computing cluster with a few hundred processors or even on a workstation for simple configurations. The desired resolution is usually limited by the computational resources. However, to compare with tower measurements of turbulence and exchange fluxes in the surface layer, a much higher resolution is required. In spite of the growth in computational power, a high-resolution LES of the surface layer is often not feasible: to fully resolve the energy-containing eddies near the surface, a grid spacing of O(1 m) is required. One way to tackle this problem is to employ a vertical grid nesting technique, in which the surface is simulated at the necessary fine grid resolution, and it is coupled with a standard, coarse, LES that resolves the turbulence in the whole boundary layer. We modified the LES model PALM (Parallelized Large-eddy simulation Model) and implemented a two-way nesting technique, with coupling in both directions between the coarse and the fine grid. The coupling algorithm has to ensure correct boundary conditions for the fine grid. Our nesting algorithm is realized by modifying the standard third-order Runge-Kutta time stepping to allow communication of data between the two grids. The two grids are concurrently advanced in time while ensuring that the sum of resolved and sub-grid-scale kinetic energy is conserved. We design a validation test and show that the temporally averaged profiles from the fine grid agree well compared to the reference simulation with high resolution in the entire domain. The overall performance and scalability of the nesting algorithm is found to be satisfactory. Our nesting results in more than 80 % savings in computational power for 5 times higher resolution in each direction in the surface layer.

UR - http://www.scopus.com/inward/record.url?scp=85068234896&partnerID=8YFLogxK

U2 - 10.5194/gmd-12-2523-2019

DO - 10.5194/gmd-12-2523-2019

M3 - Article

AN - SCOPUS:85068234896

VL - 12

SP - 2523

EP - 2538

JO - Geoscientific model development

JF - Geoscientific model development

SN - 1991-959X

IS - 6

ER -