Abstract

The heat and mass transfer over the sea is considered in terms of the sea surface roughness lengths for scalars, z 0T for potential temperature u, and z 0q for specific humidity q, or alternatively, in terms of the roughness-layer scalar increments, du and dq. A new scaling reasoning is proposed in support of the familiar square root dependence of the above increments on the roughness Reynolds number, Re0u 5 z 0uu * /n, where z 0u is the sea surface aerodynamic roughness length, u * is the friction velocity, and n is the molecular viscosity of the air. Scaling predictions are validated using data from measurements made by the National Oceanic and Atmospheric Administration’s Environmental Technology Laboratory aboard the R/V Moana Wave in the Tropical Ocean Global Atmosphere Coupled Ocean‐Atmosphere Response Experiment in 1992‐93 and the R/PFLIP in the San Clemente Ocean Probing Experiment in September 1993. Data presented as the dimensionless scalar increments (or the ratios z 0u/z 0T and z 0u/z 0q) versus Re 0u show a good agreement with theoretical predictions, especially at Re0u . 2 (over stormy sea). The resulting roughness-length formulations are recommended for practical use in climate and mesoscale air‐sea interaction models.

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