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Titlebook: Boundary-Layer Meteorology 25th Anniversary Volume, 1970–1995; Invited Reviews and J. R. Garratt,P. A. Taylor Book 1996 Springer Science+B

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Notizenaus den Ietzten Lebensjahren,.32 to 0.65 have been reported. Most of the data are, however, found in a rather narrow range between 0.39 and 0.41. Plotting all available atmospheric data against the so-called roughness Reynolds number, Reo = ..../. or against the surface Rossby number, Ro. = ./... gives no clear indication of sy
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https://doi.org/10.1007/978-94-017-0489-2ling of the coupled system of ocean and atmosphere. Knowledge of air- sea fluxes has grown, based on Monin-Obukhov similarity theory for surface boundary layers and on direct and indirect techniques of measuring the fluxes. This has been the basis for providing boundary conditions needed to couple a
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https://doi.org/10.1007/978-3-642-46886-5f instabilities associated with the characteristic strong inflection in the mean velocity profile. Mixing-layer turbulence, formed around the inflectional mean velocity profile which develops between two coflowing streams of different velocities, differs in several ways from turbulence in a surface
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A Professor with Industrial Experience, the ease with which the vertical flux contribution from surface area sources can be calculated. The flux contribution at an observation point . is found by summing the ratio of the particle vertical velocity at . to the “touchdown” velocity for particles which impact the ground within the source bo
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Ludwig Prandtl Gesammelte Abhandlungenon the analytical model of the boundary-layer height proposed by Gryning and Batchvarova (1990) and Batchvarova and Gryning (1991). The model accounts for the temperature jump and the mean vertical air motion at the top of the internal boundary-layer. Four cases from experiments in Nanticoke and Van
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