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µ * vs melt rate for u * 0 = 7 mm s - 1
25
20
15
10
5
0
0
5
10
15
20
25
Melt rate (cm da - 1 )
Fig. 4.7 The ratio of planetary scale to Obukhov length ( µ ) for a range of basal melt rates and
fixed interface stress typical of average values for Arctic sea ice
m 2 s - 2
2 x10 - 5
5x10 - 5
-
0
τ x ,
µ * = 0
-
10
τ x
µ * = 5
µ * = 25
τ y
- 20
-
30
-
40 m
Fig. 4.8 Profiles ofkinematic stress components for three values of the stabilityparameter,
µ
similar,buteventhough u 0 /
f remainsfixed,themagnitudeofdimensional z varies
as
η , which is 1, 0.60, and 0.32, respectively,for the given range of
µ . Note that
µ ,equivalentroughlytoabout25cmda 1 meltrate,thestress is
confined to the upper 15m or so of the water column, which would therefore limit
the depth to which mixing of the meltwater would reach. A new pycnocline would
rapidly form at about that level. Even with a relatively modest melt rate of about
5cmda 1 ,thedepthofmixingwouldbesignificantlyreduced.
Velocityinthesurfacelayerisobtainedinthesamewayasbeforebyintegrating
dimensionlessshearfromthevelocityatthetopoftheouterlayer
forthemaximum
V s
u 0 =
U 0 / η
(4.30)
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