Geoscience Reference
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3
3
corr = 0.89
2
2
corr = 0.78
1
1
0
0
0
5
10
15
20
25
0
0.5
1
U 10 , m/s
b T
Figure 9.3 Drag coefficient C D versus (left) wind speed U 10 and (right) breaking probability of
dominant waves b T (2.3) - for wave fields with b T
0 . 02
The right panel, however, identifies a potential problem. In this subplot, the ratio of
u sonic to u profile is plotted versus U 10 .Atthelow U 10 wind speeds, the ratio can be as large
as 3. This considerable scatter of the relative values of u shows that the physics of the
constant-flux layer could have been affected by background processes in the atmosphere
and at U 10
s the concept of the constant flux may not be valid over the ocean
as mentioned in Komen et al. ( 1994 ). This can be due to the non-stationarity and non-
homogeneity of the mean wind, which is very likely for fields of light winds (see, for
example, Figure 8 in Babanin & Makin , 2008 ), or perhaps the height of the constant-
flux layer can be less than 10m. In any case, the light-wind records were excluded from
the analysis below, as well as cases with very low breaking rates when plotting C D as a
function of breaking occurrence in Figure 9.3 .
One of the findings of Babanin & Makin ( 2008 ), based on the Lake George data, were
the limiting dependences of sea drag. These dependences envelope the Lake George data
from below:
<
4m
/
10 7 U 10 +
C D =
1
.
92
·
0
.
00096
(9.3)
and
10 7 U 10
c p
4
C D =
9
.
33
·
+
0
.
00096
,
(9.4)
whereas in open-sea observations sea-drag values below these limiters are a regular occur-
rence. Dependences (9.3) and (9.4) provide some Lake George “ideal” relationships for
C D . At this stage, it is not obvious what physical properties constitute the ideal conditions.
But almost any deviation from such conditions, at a given wind speed U 10 , causes the drag
at Lake George to increase. Babanin & Makin ( 2008 ) suggested that decrease of the drag
with respect to the ideal conditions, which exhibits itself in a number of known open-ocean
data sets, would be caused by a momentum flux back from the waves to the wind due to
long waves outrunning the wind. In Lake George, swell and such waves do not exist.
 
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