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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
3ı
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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