Koji Iwano, Naohisa Takagaki, Ryoichi Kurose and Satoru Komori. 2013. Mass transfer velocity across the breaking air–water interface at extremely high wind speeds. Tellus B 2013, 65, 21341, http://dx.doi.org/10.3402/tellusb.v65i0.21341
Three velocities of u*, U
10 and U
∞ were mistakenly overestimated by 9~19% in the evasion experiments. The mass transfer velocity k
L and correct velocities listed in should be used in all figures excluding figures 1 and 7. The correct correlations of eqs. (9), (10) and (11) between velocities and mass transfer velocity should be replaced by: 9
10
11
Fig. 10 Comparison of k L against U ∞ between laboratory and field measurements. Symbols and lines as in Fig. 8. A solid line shows the correct correlation curve of eq. (11) normalized to Sc=660 for the present laboratory measurements.
![Fig. 10 Comparison of k L against U ∞ between laboratory and field measurements. Symbols and lines as in Fig. 8. A solid line shows the correct correlation curve of eq. (11) normalized to Sc=660 for the present laboratory measurements.](/cms/asset/d8cd4dc5-d20e-4258-839d-074a6c83d331/zelb_a_11817294_f0001_ob.jpg)
Table 1. Mass transfer velocity and correct velocities
Eventually, the correlation between k L and U ∞ almost corresponds to the correlation curve of Wanninkhof and McGillis (1999) at high wind speeds as shown in the correct figure 10.