1978
DOI: 10.1016/0004-6981(78)90167-1
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Simple estimates for vertical diffusion from sources near the ground

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1979
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Cited by 252 publications
(99 citation statements)
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“…This ensures that our results are consistent with those obtained in earlier studies (Nieuwstadt and van Ulden 1978;van Ulden 1978). We used a typical value of deposition velocity equal to 0.01 m s −1 in the numerical model for SO 2 dispersion (Gryning et al 1983).…”
Section: Model Performancesupporting
confidence: 79%
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“…This ensures that our results are consistent with those obtained in earlier studies (Nieuwstadt and van Ulden 1978;van Ulden 1978). We used a typical value of deposition velocity equal to 0.01 m s −1 in the numerical model for SO 2 dispersion (Gryning et al 1983).…”
Section: Model Performancesupporting
confidence: 79%
“…where L is the Obukhov length defined by L = −T 0 u 3 * /(κgQ 0 ), where Q 0 is the surface kinematic heat flux, u * is the surface friction velocity, g is the acceleration due to gravity, T 0 is a reference temperature, and κ is the Von Karman constant taken to be 0.35 as in van Ulden (1978). Equation 6 is inferred from concentrations measured during the Prairie Grass experiment (Barad 1958).…”
Section: Description Of Modelsmentioning
confidence: 99%
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“…This analytical solution takes into account atmospheric stability and uses the wind velocity power law above the canopy, allowing it to be applicable to all conditions of atmospheric stability. In SAFE, the flux footprint PDF, f(x,y,z m ) in m −2 , is defined as the product of the crosswind concentration distribution function D y (x,y) in m −1 and the crosswind-integrated footprint, f y (x,z m ) in m −1 (Pasquill and Smith, 1983;van Ulden, 1978;Horst and Weil, 1992). The SAFE model input includes the EC sensor height (h m ), canopy height (h c ), roughness length (z 0 ), friction wind speed threshold for EC flux calculation (u th * ), and several meteorological variables (WD, u, v and u * ) and sensible and latent heat fluxes measured at the EC sensor height.…”
Section: Footprint Pdf Modellingmentioning
confidence: 99%
“…Analytical solution for the Eulerian and Lagrangian particle models are usually obtained just for stationary conditions and by making strong assumptions about the wind solutions of the diffusion-advection equation they are assumed constant along the whole Planetary Boundary Layer (PBL) or following a power law (van Ulden, 1978;Pasquill and Smith, 1983;Seinfeld, 1986;Tirabassi et al, 1986;Sharan et al, 1996). In Lagrangian particle models, the solution of the Langevin equation is normally obtained according to the rules is normally obtained according to the rules of the Ito calculus (Rodean, 1996).…”
Section: Introductionmentioning
confidence: 99%