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Featured researches published by Jeffrey Weil.


Boundary-Layer Meteorology | 1992

Footprint estimation for scalar flux measurements in the atmospheric surface layer

Thomas W. Horst; Jeffrey Weil

The flux footprint is the contribution, per unit emission, of each element of a surface area source to the vertical scalar flux measured at height zm; it is equal to the vertical flux from a unit surface point source. The dependence of the flux footprint on crosswind location is shown to be identical to the crosswind concentration distribution for a unit surface point source; an analytic dispersion model is used to estimate the crosswind-integrated flux footprint. Based on the analytic dispersion model, a normalized crosswind-integrated footprint is proposed that principally depends on the single variable z/zm, where z is a measure of vertical dispersion from a surface source. The explicit dependence of the crosswind-integrated flux footprint on downwind distance, thermal stability and surface roughness is contained in the dependence of z on these variables. By also calculating the flux footprint with a Lagrangian stochastic dispersion model, it is shown that the normalized flux footprint is insensitive to the analytic model assumption of a self-similar vertical concentration profile.


Journal of Applied Meteorology | 2005

AERMOD: A Dispersion Model for Industrial Source Applications. Part I: General Model Formulation and Boundary Layer Characterization

Alan J. Cimorelli; Steven G. Perry; Akula Venkatram; Jeffrey Weil; Robert J. Paine; Robert B. Wilson; Russell F. Lee; Warren D. Peters; Roger W. Brode

Abstract The formulation of the American Meteorological Society (AMS) and U.S. Environmental Protection Agency (EPA) Regulatory Model (AERMOD) Improvement Committee’s applied air dispersion model is described. This is the first of two articles describing the model and its performance. Part I includes AERMOD’s characterization of the boundary layer with computation of the Monin–Obukhov length, surface friction velocity, surface roughness length, sensible heat flux, convective scaling velocity, and both the shear- and convection-driven mixing heights. These parameters are used in conjunction with meteorological measurements to characterize the vertical structure of the wind, temperature, and turbulence. AERMOD’s method for considering both the vertical inhomogeneity of the meteorological characteristics and the influence of terrain are explained. The model’s concentration estimates are based on a steady-state plume approach with significant improvements over commonly applied regulatory dispersion models. Co...


Journal of Atmospheric and Oceanic Technology | 1994

How Far is Far Enough?: The Fetch Requirements for Micrometeorological Measurement of Surface Fluxes

T. W. Horst; Jeffrey Weil

Abstract Recent model estimates of the flux footprint are used to examine the fetch requirements for accurate micro-meteorological measurement of surface fluxes of passive, conservative scalars within the surface flux layer. The required fetch is quantified by specifying an acceptable ratio of the measured flux to the local surface flux. When normalized by the measurement height zm, the fetch is found to be a strong function of atmospheric stability as quantified by zm/L, where L is the Obukhov length, and a weaker function of the normalized measurement height zm/zo, where zo is the roughness length. Stable conditions are found to require a much greater fetch than do unstable conditions, and the fetch required for even moderately stable conditions is for many situations considerably greater than 100 times the measurement height.


Boundary-Layer Meteorology | 1999

An Analytical one-Dimensional Second-Order Closure Model of Turbulence Statistics and the Lagrangian Time Scale Within and Above Plant Canopies of Arbitrary Structure

William J. Massman; Jeffrey Weil

An analytical one-dimensional second-order closure model is developed to describe the within canopy velocity variances, turbulent intensities, dissipation rates, Lagrangian time scale and Lagrangian far field diffusivities for vegetation canopies of arbitrary structure and density. The model incorporates and extends the model of momentum transfer developed by Massman (1997) and the model of within canopy velocity variances developed by Weil (unpublished) from the second-order closure model of Wilson and Shaw (1977). Model predictions of within and above canopy velocity variances, turbulent intensities, dissipation rates and the Lagrangian time scale are in reasonable agreement with previously measured or estimated values for these parameters. The present model suggests that the Lagrangian time scale and the far field diffusivity could be strongly dependent upon foliage structure and density through the foliage effects on the velocity variances. A simple formulation for the Lagrangian time scale at canopy height is derived from model results. Taken as a whole, the present model may provide a relatively simple way to incorporate turbulence parameters into models of soil/canopy/atmosphere mass transfer.


Journal of the Atmospheric Sciences | 1990

A diagnosis of the asymmetry in top-down and bottom-up diffusion using a Lagrangian stochastic model

Jeffrey Weil

Abstract A Lagrangian stochastic model of particle trajectories is used to investigate the asymmetry in vertical diffusion from area sources at the bottom and top of an inhomogeneous turbulent boundary layer. Such an asymmetry was discovered in the large-eddy simulations (LES) of the convective boundary layer (CBL) by Wyngaard and Brost (1984) and Moeng and Wyngaard (1984). For inhomogeneous Gaussian turbulence, a diffusion asymmetry results from the vertical asymmetry in the vertical velocity variance about the midplane of the boundary layer. For small turbulence time scales, this is predictable from eddy-diffusion (K) theory. However, for large time scales, K theory is inapplicable as evidenced by countergradient flux regions and K singularities. The fundamental causes of the K model breakdown are the memory (large time scale) and vertical inhomogeneity of the turbulence, which lead to a mean vertical acceleration of particles away from the source and a “drift” velocity. A positive skewness in vertical ...


Journal of Applied Meteorology | 2005

AERMOD: A Dispersion Model for Industrial Source Applications. Part II: Model Performance against 17 Field Study Databases

Steven G. Perry; Alan J. Cimorelli; Robert J. Paine; Roger W. Brode; Jeffrey Weil; Akula Venkatram; Robert B. Wilson; Russell F. Lee; Warren D. Peters

Abstract The performance of the American Meteorological Society (AMS) and U.S. Environmental Protection Agency (EPA) Regulatory Model (AERMOD) Improvement Committee’s applied air dispersion model against 17 field study databases is described. AERMOD is a steady-state plume model with significant improvements over commonly applied regulatory models. The databases are characterized, and the performance measures are described. Emphasis is placed on statistics that demonstrate the model’s abilities to reproduce the upper end of the concentration distribution. This is most important for applied regulatory modeling. The field measurements are characterized by flat and complex terrain, urban and rural conditions, and elevated and surface releases with and without building wake effects. As is indicated by comparisons of modeled and observed concentration distributions, with few exceptions AERMOD’s performance is superior to that of the other applied models tested. This is the second of two articles, with the firs...


Journal of Applied Meteorology | 1992

Evaluating Air-Quality Models: Review and Outlook

Jeffrey Weil; R. I. Sykes; Akula Venkatram

Abstract Over the past decade, much attention has been devoted to the evaluation of air-quality models with emphasis on model performance in predicting the high concentrations that are important in air-quality regulations. This paper stems from our belief that this practice needs to be expanded to 1) evaluate model physics and 2) deal with the large natural or stochastic variability in concentration. The variability is represented by the root-mean- square fluctuating concentration (σc about the mean concentration (C) over an ensemble—a given set of meteorological, source, etc. conditions. Most air-quality models used in applications predict C, whereas observations are individual realizations drawn from an ensemble. For σc∼C large residuals exist between predicted and observed concentrations, which confuse model evaluations. This paper addresses ways of evaluating model physics in light of the large σc the focus is on elevated point-source models. Evaluation of model physics requires the separation of the ...


Journal of Fluid Mechanics | 2003

Structure of subfilter-scale fluxes in the atmospheric surface layer with application to large-eddy simulation modelling

Peter P. Sullivan; Thomas W. Horst; Donald H. Lenschow; Chin-Hoh Moeng; Jeffrey Weil

In the atmospheric surface layer, the wavelength of the peak in the vertical velocity spectrum


Journal of the Atmospheric Sciences | 2004

The Use of Large-Eddy Simulations in Lagrangian Particle Dispersion Models

Jeffrey Weil; Peter P. Sullivan; Chin-Hoh Moeng

\Lambda_w


Physics of Fluids | 1991

Transport asymmetry in skewed turbulence

John C. Wyngaard; Jeffrey Weil

decreases with increasing stable stratification and proximity to the surface and this dependence constrains our ability to perform high-Reynolds-number large-eddy simulation (LES). Near the ground, the LES filter cutoff

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Peter P. Sullivan

National Center for Atmospheric Research

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Chin-Hoh Moeng

National Center for Atmospheric Research

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Edward G. Patton

National Center for Atmospheric Research

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Steven G. Perry

United States Environmental Protection Agency

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Alan J. Cimorelli

United States Environmental Protection Agency

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Donald H. Lenschow

National Center for Atmospheric Research

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Robert B. Wilson

United States Environmental Protection Agency

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Thomas W. Horst

National Center for Atmospheric Research

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