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Numerical modeling of waves for a tsunami early warning system

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<strong>Numerical</strong> <strong>modeling</strong> <strong>of</strong> <strong>waves</strong> <strong>for</strong> a <strong>tsunami</strong> <strong>early</strong> <strong>warning</strong> <strong>system</strong><br />

same, very fine grid, <strong>for</strong> 100 discrete frequencies. The total computational<br />

time is <strong>of</strong> the order <strong>of</strong> 8 minutes on an AMD Opteron 246 2GHz computer<br />

equipped with 4GB <strong>of</strong> RAM.<br />

aFourier<br />

x 10<br />

2.5<br />

−3<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

0 1 2 3 4 5 6 7 8 9 10<br />

2<br />

1.5<br />

1<br />

0.5<br />

kh<br />

0<br />

0 1 2 3 4 5 6 7 8 9 10<br />

Figure 4.6: Upper panel: amplitude spectra <strong>of</strong> the surface elevation<br />

equal to that described in caption <strong>of</strong> Figure 4.5 versus the wave length<br />

parameter. Lower panel: distribution <strong>of</strong> the wave celerities over the wave<br />

length parameter; the three vertical solid lines represent the frequencies<br />

corresponding to h/L =1/20 (blue), h/L =1/4 (green) and h/L =1/2<br />

(red).<br />

The figure 4.6 looks in more detail how the wave energy is distributed<br />

in frequency. In the upper panel the same amplitude spectra <strong>of</strong> the water<br />

level oscillation at gauge 1 is reported now versus the wave length parameter<br />

written as kh. The figure is zoomed only <strong>for</strong> those frequencies where there<br />

is the major wave energy content. In the lower panel are reported the wave<br />

celerity functions against the same wave length parameter: the solid line<br />

represents the wave celerity in the shallow water approximation (csw = √ gh),<br />

while the dash-dot line and the dashed line represent respectively the phase<br />

Università degli Studi di Roma Tre - DSIC 46<br />

kh<br />

csw<br />

cg<br />

c

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