The resulting regression lines for the mean square slopes σu2 and σc2 demonstrate a nearly Selleckchem Daporinad linear dependence on the wind speed U10 at the standard height of 10 m above the sea surface (see Figure 1): equation(1) σu2=0.000+3.16×10−3U10σc2=0.0028+1.88×10−3U10}.Subscripts c and u refer to the cross-wind and up-wind directions respectively, and the coefficients 3.16 and 1.88 have the dimension [s m−1]. The ratio of the mean square of the cross-wind and up-wind slope components varies between 0.54 and 1.0, with a mean value of 0.75. The authors found that the presence of oil slicks tends to suppress the shorter waves

and reduce the mean square slope by a factor of 2 to 3. Pelevin & Burtsev see more (1957) published results of their experiment in the coastal region of the Black Sea. They confirmed Cox & Munk’s nearly linear dependence of the sea surface slope on the wind speed. For the mean square slopes they obtained equation(2) σu2=−0.0033+2.48×10−3U10σc2=0.00196+1.96×10−3U10}.The coefficients 2.48 and 1.96 have the dimension [s m−1]. The wind speed and wind

fetch during the experiment varied from 4 m s−1 to 7 m s−1, and from 30 km to 100 km, respectively. It is obvious that the observed sea surface slope depends on the intensity of the atmosphere-sea interaction. To include this phenomenon in the statistics of surface slopes, Woźniak (1996) introduced to the analysis the mean wave height H¯ instead of the wind speed U10. In particular, let us assume a Molecular motor very large wind fetch X. Thus, we obtain ( Krylov et al. 1976) equation(3) gH¯U102≈0.16and equation(4) U102=g0.16H¯≈61H¯.In fact, Woźniak used a slightly different relationship, based on the SMB method ( Massel 1996), namely: equation(5) U102≈55.64H¯. Hughes et al. (1977) combined optical, television and digital electronic techniques to design a fast response instrument for the measurement of sea

surface slope. The data taken with the fully corrected, properly adjusted instrument from the Bute Inlet-George Strait indicate that the ratio of the mean square slopes σc2/σu2 varies from 0.50 to 0.80 for wind speeds from 4 to 8 m s−1. No obvious trend in σc2/σu2 with wind speed has been observed. However, the third- and fourth-order moments in the Gram-Charlier probability distribution determined for nine data samples compared favourably with the earlier measurements by Cox & Munk (1954). Observed surface wave spectra include a large variety of wavelengths, from very short capillary waves to long swell. The very short waves are usually superimposed on the long waves, which form a background for them.