Numerical modeling of waves for a tsunami early warning system
Numerical modeling of waves for a tsunami early warning system
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 />
is even more accentuated: it is easy to distinguish a first wave train, which<br />
almost perfectly superimpose the laboratory measurement, and a second one<br />
which appears only in the numerical model results.<br />
ηS6(m)<br />
ηS9(m)<br />
0.01<br />
0.005<br />
0<br />
−0.005<br />
−0.01<br />
0.01<br />
0.005<br />
0<br />
−0.005<br />
−0.01<br />
15 20 25 30 35 40<br />
15 20 25 30 35 40<br />
t(s)<br />
ηS13(m)<br />
0.01<br />
0.005<br />
0<br />
−0.005<br />
−0.01<br />
15 20 25 30 35 40<br />
t(s)<br />
Figure 4.33: Comparison <strong>of</strong> the free surface elevations at the back field gauges<br />
position, measured (red dashed line) and obtained from the numerical model<br />
(black solid line). The numerical results are achieved by using the registration<br />
<strong>of</strong> the free surface elevation at the gauge 12S to estimate the wave source<br />
term.<br />
SS12<br />
3000<br />
2000<br />
1000<br />
0<br />
0 1 2 3<br />
f (Hz)<br />
SS15<br />
3000<br />
2000<br />
1000<br />
0<br />
0 1 2 3<br />
f (Hz)<br />
Figure 4.34: Comparison <strong>of</strong> the wave energy spectra at gauges 12S (left<br />
panel) and 15S (right panel), measured (red dashed line) and obtained from<br />
the numerical model (black solid line). The numerical results are achieved<br />
by using the registration <strong>of</strong> the free surface elevation at the gauge 12S to<br />
estimate the wave source term.<br />
Università degli Studi di Roma Tre - DSIC 79