Large-eddy Simulations of the Convective and Evening Transition Planetary Boundary Layers

Large-eddy Simulations of the Convective and Evening Transition Planetary Boundary Layers PDF Author: David Scot DeCroix
Publisher:
ISBN:
Category :
Languages : en
Pages : 275

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Book Description
Keywords: large eddy simulation, turbulence, planetary boundary layer, convective boundary layer, turbulence decay.

Large-eddy Simulations of the Convective and Evening Transition Planetary Boundary Layers

Large-eddy Simulations of the Convective and Evening Transition Planetary Boundary Layers PDF Author: David Scot DeCroix
Publisher:
ISBN:
Category :
Languages : en
Pages : 275

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Book Description
Keywords: large eddy simulation, turbulence, planetary boundary layer, convective boundary layer, turbulence decay.

Large-eddy Simulations of the Convective and Evening Transition Planetary Boundary Layers

Large-eddy Simulations of the Convective and Evening Transition Planetary Boundary Layers PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
Large-eddy simulation (LES) is a very useful tool in computationalfluid dynamics. The LES model allows one to solve a filtered set of theNavier-Stokes equations, thereby explicitly resolving scales of motionlarger than the discretization or grid size. Those motions smaller thanthe grid size are parameterized using a so-called subgrid scale model. In this series of papers, we will use the TASS LES model, originallya cloud model, which has been modified to simulate planetary boundarylayer turbulence. We will first introduce the LES model and a newgrid-nesting method for the LES. Then we will present simulations ofthe convective planetary boundary layer, and then use the LES to studythe decay of convective planetary boundary layer turbulence to a stablystratified state. The LES model has been modified to include a grid nesting capability. Grid meshes of higher resolution may be embedded within the LES enablingone to resolve smaller scales of motion (turbulence) than would bepossible by using a single grid mesh. The grid nesting methodology isdescribed in detail in Chapter 2. In Chapter 3, the nested-grid LES will be applied to thesimulation of the convective planetary boundary layer. We will usea total of three grid meshes to increase the resolution in the surfacelayer, allowing a detailed analysis of the turbulence near the surface ofthe earth. In Chapter 4, we will focus on applying Rayleigh Benardconvection criteria, using a linearized perturbation method, to the surface layer of a CBL produced by large-eddy simulation. Similarities and differences will be discussed between the LESproduced surface layer and classical Rayleigh-Benard convection theory. In Chapter 5, using a large-eddy simulation model, we willexamine in detail the turbulent kinetic energy (TKE) budget during theevening transition. The simulation will be performed in order to compareto observations gathered at the Dallas-Fort Worth International Airport, Fort-Worth, TX. during September and October 1997.

Determination of Characteristic Turbulence Length Scales from Large Eddy Simulation of the Convective Planetary Boundary Layer

Determination of Characteristic Turbulence Length Scales from Large Eddy Simulation of the Convective Planetary Boundary Layer PDF Author: Jürgen Helmert
Publisher:
ISBN:
Category :
Languages : en
Pages : 117

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Direct and Large-Eddy Simulation X

Direct and Large-Eddy Simulation X PDF Author: Dimokratis G.E. Grigoriadis
Publisher: Springer
ISBN: 3319632124
Category : Technology & Engineering
Languages : en
Pages : 523

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Book Description
This book addresses nearly all aspects of the state of the art in LES & DNS of turbulent flows, ranging from flows in biological systems and the environment to external aerodynamics, domestic and centralized energy production, combustion, propulsion as well as applications of industrial interest. Following the advances in increased computational power and efficiency, several contributions are devoted to LES & DNS of challenging applications, mainly in the area of turbomachinery, including flame modeling, combustion processes and aeroacoustics. The book includes work presented at the tenth Workshop on 'Direct and Large-Eddy Simulation' (DLES-10), which was hosted in Cyprus by the University of Cyprus, from May 27 to 29, 2015. The goal of the workshop was to establish a state of the art in DNS, LES and related techniques for the computation and modeling of turbulent and transitional flows. The book is of interest to scientists and engineers, both in the early stages of their career and at a more senior level.

Large-eddy Simulation

Large-eddy Simulation PDF Author: Working Group on Large-Eddy Simulation (Boulder, Colo.)
Publisher:
ISBN:
Category : Atmospheric turbulence
Languages : en
Pages : 122

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Large-eddy Simulation of the Nighttime Stable Atmospheric Boundary Layer

Large-eddy Simulation of the Nighttime Stable Atmospheric Boundary Layer PDF Author: Bowen Zhou
Publisher:
ISBN:
Category :
Languages : en
Pages : 350

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Book Description
A stable atmospheric boundary layer (ABL) develops over land at night due to radiative surface cooling. The state of turbulence in the stable boundary layer (SBL) is determined by the competing forcings of shear production and buoyancy destruction. When both forcings are comparable in strength, the SBL falls into an intermittently turbulent state, where intense turbulent bursts emerge sporadically from an overall quiescent background. This usually occurs on clear nights with weak winds when the SBL is strongly stable. Although turbulent bursts are generally short-lived (half an hour or less), their impact on the SBL is significant since they are responsible for most of the turbulent mixing. The nighttime SBL can be modeled with large-eddy simulation (LES). LES is a turbulence-resolving numerical approach which separates the large-scale energy-containing eddies from the smaller ones based on application of a spatial filter. While the large eddies are explicitly resolved, the small ones are represented by a subfilter-scale (SFS) stress model. Simulation of the SBL is more challenging than the daytime convective boundary layer (CBL) because nighttime turbulent motions are limited by buoyancy stratification, thus requiring fine grid resolution at the cost of immense computational resources. The intermittently turbulent SBL adds additional levels of complexity, requiring the model to not only sustain resolved turbulence during quiescent periods, but also to transition into a turbulent state under appropriate conditions. As a result, LES of the strongly stable SBL potentially requires even finer grid resolution, and has seldom been attempted. This dissertation takes a different approach. By improving the SFS representation of turbulence with a more sophisticated model, intermittently turbulent SBL is simulated, to our knowledge, for the first time in the LES literature. The turbulence closure is the dynamic reconstruction model (DRM), applied under an explicit filtering and reconstruction LES framework. The DRM is a mixed model that consists of subgrid scale (SGS) and resolved subfilter scale (RSFS) components. The RSFS portion is represented by a scale-similarity model that allows for backscatter of energy from the SFS to the mean flow. Compared to conventional closures, the DRM is able to sustain resolved turbulence under moderate stability at coarser resolution (thus saving computational resources). The DRM performs equally well at fine resolution. Under strong stability, the DRM simulates an intermittently turbulent SBL, whereas conventional closures predict false laminar flows. The improved simulation methodology of the SBL has many potential applications in the area of wind energy, numerical weather prediction, pollution modeling and so on. The SBL is first simulated over idealized flat terrain with prescribed forcings and periodic lateral boundaries. A wide range of stability regimes, from weakly to strongly stable conditions, is tested to evaluate model performance. Under strongly stable conditions, intermittency due to mean shear and turbulence interactions is simulated and analyzed. Furthermore, results of the strongly stable SBL are used to improve wind farm siting and nighttime operations. Moving away from the idealized setting, the SBL is simulated over relatively flat terrain at a Kansas site over the Great Plains, where the Cooperative Atmospheric-Surface Exchange Study - 1999 (CASES-99) took place. The LES obtains realistic initial and lateral boundary conditions from a meso-scale model reanalysis through a grid nesting procedure. Shear-instability induced intermittency observed on the night of Oct 5th during CASES-99 is reproduced to good temporal and magnitude agreement. The LES locates the origin of the shear-instability waves in a shallow upwind valley, and uncovers the intermittency mechanism to be wave breaking over a standing wave (formed over a stagnant cold-air bubble) across the valley. Finally, flow over the highly complex terrain of the Owens Valley in California is modeled with a similar nesting procedure. The LES results are validated with observation data from the 2006 Terrain-Induced Rotor Experiment (T-REX). The nested LES reproduces a transient nighttime warming event observed on the valley floor on April 17 during T-REX. The intermittency mechanism is shown to be through slope-valley flow transitions. In addition, a cold-air intrusion from the eastern valley sidewall is simulated. This generates an easterly cross-valley flow, and the associated top-down mixing through breaking Kelvin-Helmholtz billows is analyzed. Finally, the nesting methodology tested and optimized in the CASES-99 and T-REX studies is transferrable to general ABL applications. For example, a nested LES is performed to model daytime methane plume dispersion over a landfill and good results are obtained.

Large Eddy Simultations of the Atmospheric Boundary Layer East of the Colorado Rockies

Large Eddy Simultations of the Atmospheric Boundary Layer East of the Colorado Rockies PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 140

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Book Description
Large eddy simulation, LES, has often been carried out for the idealized situation of a simple convective boundary layer. Studies of dual Doppler radar and aircraft data from the Phoenix II experiment indicate that the boundary layer of the Colorado High Plains is not a purely convective boundary layer and it is influenced by the mountains to the west. The purpose of this study is to investigate the atmospheric boundary layer on one particular day on the Colorado High Plains. This research applies a LES nested within larger grids, which contain realistic topography and can simulate the larger-scale circulations initiated by the presence of the mountain barrier. How and to what extent the atmospheric boundary layer of the Colorado High Plains is influenced by larger scale circulations and other phenomena associated with the mountain barrier to the west is investigated. The nested grid LES reproduces the characteristics of the atmosphere for the case study day reasonably well. The mountains influence the atmospheric boundary layer over the plains to the east in several ways. The mountains contribute to the vertical shear of the horizontal winds through the thermally-induced mountain-plains circulation. As a consequence of the wind shear, the boundary layer that develops over the mountains is advected eastward over the top of the plains boundary layer, which is developing separately. This layer is marked by a mixture of gravity waves and turbulence and is atypical of a purely convective boundary layer. Just below this layer, the capping inversion of the plains boundary layer is weak and poorly defined compared to the inversions capping purely convective boundary layers. Gravity waves, triggered by the obstacle of the Rocky Mountains and by convection in the mountain boundary layer, also influence the atmosphere above the Colorado High Plains. These influences are found to have significant effects on the turbulence statistics and the energy spectra.

Large-eddy Simulation of the Convective Boundary Layer

Large-eddy Simulation of the Convective Boundary Layer PDF Author: Frans T. M. Nieuwstadt
Publisher:
ISBN:
Category :
Languages : en
Pages : 495

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The Atmosphere and Climate of Mars

The Atmosphere and Climate of Mars PDF Author: Robert M. Haberle
Publisher: Cambridge University Press
ISBN: 110817938X
Category : Science
Languages : en
Pages : 613

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Book Description
Humanity has long been fascinated by the planet Mars. Was its climate ever conducive to life? What is the atmosphere like today and why did it change so dramatically over time? Eleven spacecraft have successfully flown to Mars since the Viking mission of the 1970s and early 1980s. These orbiters, landers and rovers have generated vast amounts of data that now span a Martian decade (roughly eighteen years). This new volume brings together the many new ideas about the atmosphere and climate system that have emerged, including the complex interplay of the volatile and dust cycles, the atmosphere-surface interactions that connect them over time, and the diversity of the planet's environment and its complex history. Including tutorials and explanations of complicated ideas, students, researchers and non-specialists alike are able to use this resource to gain a thorough and up-to-date understanding of this most Earth-like of planetary neighbours.

Simulating the Evening Transition in the PbL and Evaluating Its Contribution to the Next Day Prediction Ozone Peak Concentration

Simulating the Evening Transition in the PbL and Evaluating Its Contribution to the Next Day Prediction Ozone Peak Concentration PDF Author: Gustavo Copstein Cuchiara
Publisher:
ISBN:
Category : Air quality
Languages : en
Pages :

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Book Description
The transition from the convective boundary layer during the daytime to the stable stratified boundary layer during nighttime after sunset plays an important role in the transport and dispersion of atmospheric pollutants. However, our knowledge regarding this transition and its feedback on the structure of the subsequent nocturnal boundary layer is still restricted. This also prevents forecast models from accurate prediction of the onset and development of the nighttime boundary layer, which determines the redistribution of pollutants within the nocturnal surface layer and the residual layer aloft. Turbulence in the stable nocturnal boundary layer is generally weak and typically characterized by intermittent bursts of activity. It often exists in isolated layers generated primarily from localized shear instabilities. As a result, turbulence is rarely in equilibrium with the conditions of the underlying surface. Given the layered structure of the nocturnal boundary layer, the spatial and temporal characteristics of turbulent activity can have a significant effect on local air quality at hourly to diurnal scales. In a case study using Large-Eddy Simulation was found a weak, but noticeable nighttime turbulent kinetic energy produced by wind shear in Houston’s planetary boundary layer (PBL). This may likely be related to observations made at the UH Moody Tower on at least two Vertical Mixing Experiment days, when peaks of carbon monoxide occurred in the evening, while the variability in wind conditions was very little. This supports a hypothesis of intermittent turbulence acting in the concentration of pollutants measured at the UH Moody Tower air quality station The overall goal of this study was to improve the current understanding of dynamical processes of the diurnal cycle of the PBL that impacts the vertical distribution of pollutants, with particular attention to the representation of the late afternoon in meteorological and air quality models. This goal was assessed throughout the sensitivity analysis of a more realistically representation of diffusion process during the decay of the convective boundary layer, typical of the evening transition, in a widely-used weather and air quality forecast model (WRF/Chem). Improvements in O3 precursors were possible without a significant increase in complexity or computer time.