For a scientific approach to extreme events Asymptotic analysis of typhoons and tsunami Daniela...
-
Upload
anais-rowlett -
Category
Documents
-
view
219 -
download
0
Transcript of For a scientific approach to extreme events Asymptotic analysis of typhoons and tsunami Daniela...
For a scientific approach to extreme events
Asymptotic analysis of typhoons and tsunami
Daniela Bianchi , Department of Physics, Univ. Of Rome “La Sapienza”
Sergey Dobrokhotov, Institute of Problem of Mechanics, Moscow Academy of Sciences
Fabio Raicich, ISMAR , CNR Trieste
Sergiy Reutskiy, Ukrainian Academy of Science, Kharkov
Brunello Tirozzi , Department of Physics, Univ. Of Rome “La Sapienza”
Poleward heat transport
Wind system for water covered Earth
Main wind system (Northern summer)
Main wind system (Southern summer)
Cyclon and Anticyclon
Cyclogenesis at mid latitudes
Westerlies-Rossby wave
Nanmadol
Forecast without heat exchange
Sonca
Forecast without heat exchange
Kirogi
1000 500 500 1000x
1000
500
500
1000
q
Real and computed trajectory with heat exchange
Real and forecast trajectory
Maslov decomposition (1/2)
x is the difference among the running point and the typhoon center
F is a function with the singularity in the origin of the square root type
S is a quadratic function of the coordinates x with different eigenvalues
f(x,t), g(x,t) are smooth functions
Self-similarity and stability properties
Maslov decomposition (2/2)
Cauchy Riemann conditions and
stability of perturbations
Perturbed solutions of SW equations (1/3)
Perturbed solutions of SW equations (2/3)
Perturbed solutions of SW equations (3/3)
Conserved structure of the solution (1/2)
Conserved structure of the solution (2/2)
Chi variable at each 0.25 degrees for the 00 of 18.09.06
Sanshan positions: 37.1 N, 132.4 E (developed)
Yagi positions: 20.5 N, 158.6 E (beginning)1 : Chi =0.1282 sec^(-1)
Computation of the trajectory of the center of typhoons
SW+temp. eq. (1/2)
Sw+temp.eq (2/2)
Lax Wendroff Method (1/4)
Lax Wendroff method (2/4)
Lax Wendroff method (3/4)
Lax-Wendroff Method (4/4)
Stability of the vortex
Non stability of the vortex
Boundary conditions (1/3)
Boundary conditions (2/3)
Boundary conditions (3/3)
Neural Network (1/4)
Neural Network (2/4)
Neural Network (3/4)
Neural Network (4/4)
Hugoniot-Maslov Hierarchy 1/15
Hugoniot-Maslov Hierarchy 2/15
Hugoniòt-Maslov Hierarchy 3/15
Hugoniòt-Maslov Hierarchy 4/15
Hugoniòt-Maslov Hierarchy 5/15
Hugoniòt-Maslov Hierarchy 6/15
Hugoniòt-Maslov Hierarchy 7/15
Hugoniòt-Maslov Hierarchy 8/15
Hugoniòt-Maslov Hierarchy 9/15
Hugoniòt-Maslov Hierarchy 10/15
Hugoniòt-Maslov Hierarchy 11/15
Hugoniòt-Maslov Hierarchy 12/15
Hugoniòt-Maslov Hierarchy 13/15
Hugoniòt-Maslov Hierarchy 14/15
Hugoniòt-Maslov Hierarchy 15/15
More phenomenology (1/4)
More phenomenology (2/4)
More phenomenology (3/4)
More phenomenology (4/4)
Workshop On Renormalization Group, Kyoto 2005
B. Tirozzi, S.Yu. Dobrokhotov,
S.Ya. Sekerzh-Zenkovich,
T.Ya. Tudorovskiy
Analytical and numerical analysis of the wave profiles near the fronts appearing in
Tsunami problems
“Gaussian” source of Earthquake
-5
-2.5
0
2.5
5-5
-2.5
0
2.5
5
00.250.5
0.751
-5
-2.5
0
2.5
5
Level curves of perturbation
-2-1
01
2
-4-2
024
Wave profiles at the front at time t at different angles
-4 -2 2 4
-0.5
0.5
1
1.5
3D wave profile for elliptic source
-20
-10
0
10
20-20
-10
0
10
20
-0.500.511.5
-20
-10
0
10
20
“Modulated gaussian” source of Earthquake
-5
-2.5
0
2.5
5-5
-2.5
0
2.5
5
-2
0
2
-5
-2.5
0
2.5
5
Level curves of perturbation
-2-1
01
2
-4-2
024
Wave profiles at the front at time t at different angles
-4 -2 2 4
-1
-0.75
-0.5
-0.25
0.25
0.5
0.75
1
3D wave profile for elliptic source
-20
-10
0
10
20-20
-10
0
10
20
-2-1012
-20
-10
0
10
20
The ridge near the source of Eathquake
-5
0
5
-5
0
5
-3
-2
-1
0
-5
0
5-6 -4 -2 0 2 4 6
-6
-4
-2
0
2
4
6
Fronts at different times
The set of profiles
-20 -15 -10 -5 5 10 15 20
-20
-15
-10
-5
5
10
15
20
0.658889
1.48386
1.03988
0.0444183
1.03364
1.47197
0.658554
0.00228282
-20 -15 -10 -5 5 10 15 20
-20
-15
-10
-5
5
10
15
20
0.658889
1.48386
1.03988
0.0444183
1.03364
1.47197
0.658554
0.00228282
Simulations for Tyrrhenian Sea
-400 -200 0 200 400
-400
-200
0
200
400
-400 -200 0 200 400
-400
-200
0
200
400
Relief data:National Oceanic and Atmospheric Administration (NOAA)National Geophysical Data Center (NGDC)ETOPO2 2-minute Global Reliefhttp://www.ngdc.noaa.gov/mgg/gdas/gd_designagrid.html
Rays for imaginary source at Stromboli: 38.8 N, 15.2 E
50 100 150 200 250 300 350 400
-400
-350
-300
-250
-200
-150
-100
-50
Amplitudes of wave at different points of the coast
150 200 250 300 350 400 450
-350
-300
-250
-200
-150
-100
0.155356
0.0916952
0.118962
0.019779
0.00317829
0.09830570.0886875
0.306578
0.1297210.00840296
3D wave profile
Density plot
... Workshop on Extreme Events ...Max Planck Institut for Complex SystemDresden, 30 October-2 November 2006
Analysis of the tsunami event in Algeria 2003
S. Dobrokhotov (1), B. Tirozzi (2), P. Zhevandrov (3),
F. Raicich (4)
(1) Institute for Problems in Mechanics, RAS, Moscow, Russia(2) Department of Physics, University “La Sapienza”, Rome, Italy(3) Escuela de Ciencias Fisico-Matematicas, Morelia, Mich., Mexico(4) CNR, Institute of Marine Sciences, Trieste, Italy
Valencia
Barcelona
Ibiza
Earthquake data (USGS): t0: 18:44:19 GMT, 21 may 2003 USGS: epicenter 36.96°N, 3.63°E, M=6.9, hf=12 km Borerro: epicenter 36.90°N, 3.71°E, M=6.8, hf=10 km, strike=56°
Ellipsoidal deformation
M = 6.9
hf = 12 km
(Pelinovsky et al., 2001)
a = 34 km
b = 12 km
b56°
a
Coordinates: model gridpoints
(Dobrokhotov et al., 2006)
a1= 1.2 10-2 km-1
Gaussian*cosine deformation
= 0
a2 = 2.7 10-2 km-1
b1 = 0.5 10-2 km-2
b2 = 4.0 10-2 km-2
= 56°
Coordinates: model gridpoints
Wave equation
Average of fast oscillating solutions
Amplitude of the waves at tsunami front
Solutions before and after the scattering of the beach (1/2)
Solutions before and after the scattering of the beach (2/2)
Graphics 1
Graphics 2
Graphics 3
End