29.07.2013 Views

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

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

<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 carried out by comparison with other physical experiments (see section 4.4),<br />

which intend to reproduce the landslide generated <strong>waves</strong> using a realistic<br />

model <strong>of</strong> the landslide, and a wave tank large enough to study the wave<br />

propagation in the far field. The physical model was build at the LIAM<br />

laboratory <strong>of</strong> L’Aquila University, Italy.<br />

Section 4.5 describes other experiments carried out at the Research and<br />

Experimentation Laboratory <strong>for</strong> Coastal Defence (LIC), <strong>of</strong> the Technical<br />

University <strong>of</strong> Bari, Italy. These experiments reproduce the particular case <strong>of</strong><br />

a landslide falling at the flank <strong>of</strong> a conical island and allow the analysis <strong>of</strong><br />

the generated wave field close to the island and in the far propagation field.<br />

The physical experiments are reproduced with the numerical model which<br />

provides results in good agreement with the laboratory measurements. The<br />

numerical model is tested both with the ‘indirect’ and the ‘direct’ procedure,<br />

in order to validate its application to work in a <strong>early</strong> warnuìing <strong>system</strong> and<br />

to gain more insight on generation and propagation <strong>of</strong> <strong>tsunami</strong>s <strong>for</strong> this<br />

particular bathymetric configuration.<br />

In the end, section 4.6 presents a test case to validate the model<br />

application to large geographical areas, by means <strong>of</strong> matching the solution<br />

<strong>of</strong> the elliptic MSE with its parabolic approximation.<br />

4.1 The Scott–Russel’s wave generator<br />

The physical model reproduces the so called Scott-Russel’s wave generator<br />

(see the sketch on figure 4.1 and the picture on figure 4.2), i.e. a box falling<br />

vertically into the water (Monaghan & Kos, 2000). The wave flume is made<br />

up <strong>of</strong> steel and PVC, and is 12.00 m long, 0.30 m wide and 0.45 m high; the<br />

box (0.10 m x0.10 m x0.30 m) is made <strong>of</strong> PVC. The wave generator was<br />

placed at one end <strong>of</strong> the flume while at the other end absorbing material was<br />

used to reduce the wave reflection.<br />

The water level oscillations were measured by means <strong>of</strong> five resistive wave<br />

gauges placed along the flume, respectively at 0.40, 0.85, 1.30, 1.75 and 2.20<br />

m from the left boundary <strong>of</strong> the flume. The gauges were characterized by<br />

an instrumental noise lower than 0.1%. The data were collected using a<br />

16 channels National Instruments analog-to-digital conversion board. The<br />

recorded water level data cover a period <strong>of</strong> 20 s with a 1000 Hz sampling<br />

frequency. The experiments were carried out <strong>for</strong> four different water depths<br />

(0.06 m, 0.10 m, 0.18 m and 0.23 m), and <strong>for</strong> each <strong>of</strong> these the box was<br />

Università degli Studi di Roma Tre - DSIC 40

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!