Abstract

A challenge to simulating turbulent flow in multiscale atmospheric applications is the efficient generation of resolved turbulence motions over an area of interest. One approach is to apply small perturbations to flow variables near the inflow planes of turbulence-resolving simulation domains nested within larger mesoscale domains. While this approach has been examined in numerous idealized and simple terrain cases, its efficacy in complex terrain environments has not yet been fully explored. Here, we examine the benefits of the stochastic cell perturbation method (CPM) over real complex terrain using data from the 2017 Perdigão field campaign, conducted in an approximately 2-km wide valley situated between two nearly parallel ridges. Following a typical configuration for multiscale simulation using nested domains within the Weather Research and Forecasting (WRF) model to downscale from the mesoscale to a large-eddy simulation (LES), we apply the CPM on a domain with horizontal grid spacing of 150 m. At this resolution, spurious coherent structures are often observed under unstable atmospheric conditions with moderate mean wind speeds. Results from such an intermediate resolution grid are often nested down for finer, more detailed LES, where these spurious structures adversely affect the development of turbulence on the subsequent finer grid nest. We therefore examine the impacts of the CPM on the representation of turbulence within the nested LES domain under moderate mean flow conditions in three different stability regimes: weakly convective, strongly convective, and weakly stable. In addition, two different resolutions of the underlying terrain are used to explore the role of the complex topography itself in generating turbulent structures. We demonstrate that the CPM improves the representation of turbulence within the LES domain, relative to the use of high-resolution complex terrain alone. During the convective conditions, the CPM improves the rate at which smaller-scales of turbulence form, while also accelerating the attenuation of the spurious numerically generated roll structures near the inflow boundary. During stable conditions, the coarse mesh spacing of the intermediate LES domain used herein was insufficient to maintain resolved turbulence using CPM as the flow develops downstream, highlighting the need for yet higher resolution under even weakly stable conditions, and the importance of accurate representation of flow on intermediate LES grids.

Highlights

  • Over recent decades, computational power has grown such that it is becoming routine to perform multiscale atmospheric simulations, in which a larger-scale mesoscale flow field is dynamically downscaled using grid nesting, with finer mesh spacing over regions of interest

  • Instrumentation deployed during the Perdigão field campaign included GPS Advanced Upper-Air Sounding System (GAUSS) radiosondes as well as 195 three-component sonic anemometers and 55 temperature-humidity sensors mounted on masts of heights ranging from 2–100 m above ground level (a.g.l.) [17]

  • The simulations with and without cell perturbation method (CPM) are similar in the time series, profiles, and error statistics considered so far while more significant difference are due to the topography resolution

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Summary

Introduction

Computational power has grown such that it is becoming routine to perform multiscale atmospheric simulations, in which a larger-scale mesoscale flow field is dynamically downscaled using grid nesting, with finer mesh spacing over regions of interest. Goodfriend et al [1], in a computational fluid dynamics code, and Mirocha et al [2], using a numerical weather prediction (NWP) model, explored the transition distance required for turbulence to be generated at a coarse-to-fine grid interface. Both studies found that it takes significant fetch to sufficiently develop turbulence compared to stand-alone periodic simulations at the finer resolution, and that this fetch depends on the chosen turbulence closure model. In addition to issues of induced periodicity, periodic boundary conditions could not be used for nested simulations which must be forced by their parent at the boundary

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