After the 21 May 2003 Algiers earthquake (CSEM-EMSC
special page), sea disturbances have been observed on the southeastern
coast of the Majorca and Menorca Islands, as well as in Ibiza (Baleares).
Witnesses have reported waves up to 2 m high, and a mean period of 10-12
min in Majorca (see here).
Tide gage records are available in Palma (Figure 1), showing a maximum
water height of about 60 cm (or peak-to-trough amplitude of 1.2 meter).
Figure 1: Tide gage record in Majorca, courtesy of María
Jesús Garcia (IEO)
These sea level variations can be related to a tsunami that could have
been triggered either by the coseismic seafloor deformation induced by
the submarine fault involved in the earthquake, or by a submarine landslide.
In a first attempt we test here a source due to a coseismic seafloor
deformation, that can be estimated through a model of elastic dislocation
(Okada, 1985). This initial seafloor deformation is computed (Figure
2) with the following parameters taken from Harvard
CMT solution. The mean displacement on the fault plane is about 85
cm.
The first slip distributions obtained from seismological inversions
show that the depth was probably shallower than the one we used here, therefore
the initial seafloor displacement is probably larger than what is displayed
in Figure 2.
Fault dimensions (km x km)
40 x 20
Strike, dip, rake
56°, 46°, 71°
Seismic moment (Nm)
0.201 1020
Rigidity (Nm2)
30 109
Epicenter
3.52°E - 36.98°N
Depth (km)
17
Figure 2: Initial seafloor deformation computed with the parameters
above.
Note the small negative deformation compared to the positive one.
The initial deformation is assumed to be fully and instantaneously
transmitted to the sea surface, where, through restoring gravity forces,
tsunami waves begin to propagate across the sea.
Since tsunami wavelengths are much larger than the mean water depth,
we assume that the long wave theory is valid. The simulation is
performed using a finite difference method that solves the hydrodynamic
equations of continuity and of motion, including non linear terms.
Nested bathymetric grids are used to account for the wave amplification
near the coasts. Here we used data taken from the global bathymetry data
deduced from altimetry (compiled by Smith and Wessel, 1997), and we build
a 2' grid describing the western Mediterranean Sea, a 30'' grid for the
Baleares Islands, and 10'' grids for the Majorca and Menorca Islands (Figure
3).
Figure 3: Computational domain, and location of the fine grids
describing the Baleares Islands.
Results
The waves reach the Baleares Islands after a propagation of about 20
to 30 minutes, in agreement with the arrival in Palma roughly deduced
from Figure 1. As is usual in far-field tsunami propagation, the highest
energy, corresponding to the maximum water heights displayed in Figure
4, is limited to an area perpendicular to the fault strike (Hébert
et al., 2001a), posing a significant threat to the Baleares Islands for
this kind of fault azimut.
An animation of the propagation is available here (.gif
file, ~8 Mo, or low-quality .mpeg file,
530 ko).
Figure 4: Sea surface computed after a 25 min tsunami propagation.
Figure 5: Maximum water heights computed after a 1.5 h propagation.
In the Baleares, the results must be considered with caution.
They do not display a great amplification of the waves (Figures 6 and
7). Since the submarine slopes are quite steep, especially towards
Majorca (Figure 3), the tsunami waves could have been reflected, protecting
Palma from a large amplification.
However it is worth noting that the areas of (relatively) highest computed
amplification correspond to the localities where abnormal waves have been
reported, in Majorca (Porto Cristo) and Menorca (Mao). Further studies
should definitely use refined bathymetric data in the harbours to assess
the hazard in the Baleares more precisely.
Figure 6: Maximum water heights reached in Majorca.
Figure 7: Maximum water heights reached in Menorca.
Comments
The modelings carried out here are very preliminary, and use rough bathymetric
data only, especially for the fine grids. To account for the wave amplification
reported along the SE coasts of Majorca or Menorca, fine data should be
added in the bathymetric grids used for the simulation.
Anyway these modelings show that a coseismic source can explain
tsunami observations in the Baleares Islands, especially along their
SE coasts.
We note that tsunami observations along the Algerian coast have not
be reported so far, and attention must be paid to future witnesses accounts.
Finally, it is also worth mentioning that a dense and good-quality
tide gage network on the Mediterranean coasts could allow the implementation
of inversion techniques to recover the submarine coseismic deformation,
as it is performed in Japan for earthquakes located in the Nankai Trough
(e.g. Tanioka and Satake, 2001 ; Baba et al., 2002).
References
Baba, T., Y. Tanioka, P.R. Cummins and K. Uhira, The slip distribution
of the 1946 Nankai earthquake estimated from tsunami inversion using a
new plate model, Phys. Earth Plante. Int., 132, 1-3, 59-73, 2002.
Hébert, H., P. Heinrich, F. Schindelé, and A.
Piatanesi, Far-field simulation of tsunami propagation in the Pacific Ocean:
impact on the Marquesas Islands (French Polynesia), J. Geophys. Res., 106,
C5, 9161-9177, 2001.
Okada, Y., Surface deformation due to shear and tensile faults
in a half-space, Bull. Seismol. Soc. Am., 75, 1135-1154, 1985.
Smith, W.H.F., and Sandwell, D.T., Global seafloor topography
from satellite altimetry and ship depth soundings, Science, 277, 1956-1962,
1997.
Tanioka, Y., and K. Satake, Detailed coseismic slip distribution
of the 1944 Tonankai earthquake estimated from tsunami waveforms, Geophysical
Research Letters, 28, 1075-1078, 2001.
References of our laboratory on the subject
Guibourg, S., P. Heinrich and R. Roche, Numerical modeling of the
1995 Chilean tsunami. Impact on French Polynesia, Geophysical Research
Letters, 24, 775-778, 1997.
Hébert, H., P. Heinrich, F. Schindelé, and A.
Piatanesi, Far-field simulation of tsunami propagation in the Pacific Ocean:
impact on the Marquesas Islands (French Polynesia), J. Geophys. Res., 106,
C5, 9161-9177, 2001.
Hébert H., F. Schindelé, and P. Heinrich, Tsunami
risk assessment in the Marquesas Islands (French Polynesia) through numerical
modeling of recent and generic far-field events, Natural Hazards and Earth
System Sciences, 1, 233-242, 2001.
Hébert, H., A. Piatanesi, P. Heinrich, F. Schindelé,
and E. A. Okal, Numerical modeling of the September 13, 1999 landslide
and tsunami on Fatu Hiva Island (French Polynesia), Geophys. Res. Lett.,
29, 10, doi:10.1029/2001GL01374, 2002.
Heinrich, P., A. Mangeney, S. Guibourg, R. Roche, G. Boudon,
and J.-L. Cheminée, Simulation of water waves generated by a potential
debris avalanche in Montserrat, Lesser Antilles, Geophysical Research Letters,
25, 3697-3700, 1998.
Heinrich, P., F. Schindelé, S. Guibourg and P.F. Ihmlé,
Modeling of the February 1996 Peruvian tsunami, Geophysical Research Letters,
25, 2687-2690, 1998.
Heinrich, P., R. Roche, A. Mangeney and G. Boudon, Modéliser
un raz de marée créé par un volcan, La Recherche,
Mars 1999, 66-71, 1999.
Heinrich, P., S. Guibourg, A. Mangeney, and R. Roche, Numerical
modeling of a landslide-generated tsunami following a potential explosion
of the Montserrat Volcano, Physics and Chemistry of the Earth, 24, 16-168,
1999.
Heinrich, P., A. Piatanesi, E. Okal, and H. Hébert, Near-field
modeling of the July 17, 1998 event in Papua New Guinea, Geophysical Research
Letters, 27, 3037-3040, 2000.
Heinrich, P., A. Piatanesi, and H. Hébert, Efficiency
of deep submarine landslides in producing tsunamis: the 1998 Papua New
Guinea event, GJI, 145, 97-111, 2001.
Schindelé, F., D. Reymond, E. Gaucher and E.A. Okal,
Analysis and automatic processing in near-field of eight 1992-1994 tsunamigenic
earthquakes: improvements towards real-time tsunami warning, Pure and Applied
Geophysics, 144, 381-408, 1995.