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a
b
c
CNOP
CNOP
CNOP
37N
12h
37N
24h
37N
36h
31N
31N
31N
10
8
6
10
8
6
10
8
6
25N
25N
25N
4
4
4
19N
2
19N
2
19N
2
13N
13N
13N
111E
120E
129E
138E
111E
120E
129E
138E
111E
120E
129E
138E
Fig. 24.9 TC Meari (2004). The vertically integrated energies of CNOP ( shaded , units: J/kg) and
the 500 hPa stream fields for the second approach. ( a ) forecast starts at 12 h ahead, (b) forecast
starts at 24 h ahead, and ( c ) forecast starts at 36 h ahead (From Zhou and Mu 2012b )
a
b
c
CNOP
CNOP
CNOP
24h
36h
12h
39N
39N
39N
10
8
6
4
2
10
8
6
4
2
10
8
6
4
2
33N
33N
33N
27N
27N
27N
21N
21N
21N
15N
15N
15N
111E 120E 129E 138E
111E 120E 129E 138E
111E 120E 129E 138E
Fig. 24.10
Same as Fig. 24.9 , but for TC Matsa (2005) (From Zhou and Mu 2012b )
24.4
Examination of the CNOP Sensitive Areas
In Sect. 24.3 , we have studied the properties of the CNOP sensitive areas. In this
section, we will examine the efficiency of the CNOP sensitive areas with a lot of
cases by carrying out the sensitivity tests, OSSEs, and OSEs.
24.4.1
Sensitivity Tests
In this part, random initial errors are introduced into the CNOP sensitive areas, and
their impacts on the TC forecasts are explored ( Chen and Mu 2012 ). Two tropical
cyclones, Longwang (2005) and Sinlaku (2008) are studied. For comparison, the
roles of the random initial errors in the areas identified by FSV and CSV, and the
randomly selected areas are considered. Based on these four areas, experiments are
designed to determine which area have the greatest impact on TC forecasts.
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