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118 ° E
120 ° E
122 ° E
1 24 ° E
12 6 ° E
1 2 8 ° E
13 0 ° E
1 32 ° E
35
30
28 ° N
25
20
15
26 ° N
10
24 ° N
22 ° N
20 ° N
18 ° N
Fig. 8.7
Diagonal elements of B g in the Okinawa region at z
D 20
m. The actual values are
multiplied by 10 4
8.3.5
LH Experiments in 3d Setting
To check the performance of the LH0 and LH1 methods further, a larger 3d NCOM
domain is set up in the Okinawa region (Fig. 8.7 ) with horizontal resolution of 10 km
and 45 vertical levels. The state vector dimension
N
(total number of the grid points)
in this setting was 862,992.
Because of the large
, it is computationally unfeasible to directly compute all
the diagonal elements of the BEC matrix. Therefore, accuracy checks are performed
on a subset of 10,000 points, randomly distributed over the domain and the value of
h " i is estimated by averaging over these points.
The diffusion tensor is constructed in the same way that is described in
Sect. 8.3.1 , but the generating field u
N
.
x
/
is taken to be the horizontal velocity field
from an NCOM run. The value of
3 (in the vertical direction) is independent of
horizontal coordinates, but varies in the vertical as
ı z is the vertical
grid step. Figure 8.7 illustrates spatial variability of the B g diagonal elements at
z
z ,where
m. The smallest values are observed in the regions of the Kuroshio and
the Nor th E quatorial Current, where the largest velocities are observed, and the
˝ D
D 20
p det
reaches its largest values ( 8.44 ). To better test the algorithm, a relatively
small threshold value of v D 0:02
m/s is prescribed, so that diffusion is anisotropic
in more than 90 % of the grid points.
 
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