1987
DOI: 10.1007/bf00125144
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Comments and further analysis on effective roughness lengths for use in numerical three-dimensional models

Abstract: Simple calculations of the apparent roughness length for the areally averaged flow over flat but heterogeneous terrain are presented. These results could be used to specify effective roughness lengths for use in large-scale models. Some of our conclusions differ significantly from those reached recently by Andre and Blondin (1986).

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Cited by 116 publications
(65 citation statements)
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“…There has been abundant literature on the subject from back in the 1990s, mostly based on theoretical works deriving deterministic [41] or statistical [42] relationships between local and regional parameters for land-atmosphere exchange modelling. For roughness length, Wassenaar et al [43] conclude that a geometric averaging of the roughness length is performing best; this is also the scaling proposed by Taylor [44].…”
Section: Introductionmentioning
confidence: 64%
“…There has been abundant literature on the subject from back in the 1990s, mostly based on theoretical works deriving deterministic [41] or statistical [42] relationships between local and regional parameters for land-atmosphere exchange modelling. For roughness length, Wassenaar et al [43] conclude that a geometric averaging of the roughness length is performing best; this is also the scaling proposed by Taylor [44].…”
Section: Introductionmentioning
confidence: 64%
“…Station data were used for bias correction of the modelled wind. The 1-km 2 resolution was reached by transforming the wind speed to the local roughness length using the logarithmic wind profile law (Taylor 1987).…”
Section: Wind Componentsmentioning
confidence: 99%
“…The result for surface roughness, however, is quite different (Taylor, 1987). This method yields a grid-averaged roughness length scale which corresponds to an algebraic average of the friction velocity over the grid, and has been in fairly common use for several decades (Kung, 1963;Vihma and Savijarvi, 1991 Richardson number represents the ratio between buoyant and shear production of turbulent kinetic energy and is given by the relationship:…”
Section: Surface Moisture Availabilitymentioning
confidence: 99%