The thermal structure of an air-water interface at low wind speeds

Citation
Ra. Handler et al., The thermal structure of an air-water interface at low wind speeds, TELLUS A, 53(2), 2001, pp. 233-244
Citations number
30
Categorie Soggetti
Earth Sciences
Journal title
TELLUS SERIES A-DYNAMIC METEOROLOGY AND OCEANOGRAPHY
ISSN journal
02806495 → ACNP
Volume
53
Issue
2
Year of publication
2001
Pages
233 - 244
Database
ISI
SICI code
0280-6495(200103)53:2<233:TTSOAA>2.0.ZU;2-Q
Abstract
High-resolution infrared imagery of an air-water interface at wind speeds o f 1 to 4 ms(-1) was obtained. Spectral analysis of the data reveals several important features of the thermal structure of the so-called cool skin. At wind speeds for which wind waves are not generated, the interfacial bounda ry layer appears to be composed of buoyant plumes that are stretched by the surface shear as they reach the interface. The plumes appear to form overl apping laminae with a head-tail structure which we have termed fish-scales. At higher wind speeds, gravity waves appearing on the surface give rise to distinct signatures in the infrared imagery. The wave system appears to mo dulate the surface temperature with sufficient strength so that the length and time scales of the waves are readily revealed in a k-omega spectrum. A surface drift speed can also be easily inferred from the spectrum. A direct numerical simulation of the cool-skin of a sheared water interface has als o been performed. For Richardson numbers less than about 10(-3) the simulat ions reveal a surface temperature pattern dominated by a streaky structure with a characteristic spanwise length scale on the order of 100/(+) where l (+) = nu /u*. The simulations confirm that this streaky structure is formed as slow moving fluid originating from below encounters a surface shear. Th e thermal structure of the surface appears virtually unchanged when buoyanc y is turned off in the simulations and shear remains. This indicates that t he fish-scale pattern has universal features in the sense that it forms ind ependently of the mechanism by which the turbulence is generated. The simul ations are found to be in remarkable agreement with the experimental result s for which the same streaky, fish-scale structure was observed and the sam e streak spacing was obtained.