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Tsunami Modeling and Data Products for Early Warning

Sven Harig, Antonia Immerz, Natalja Rakowsky, Alexey Androsov, Wolfgang Hiller

Alfred Wegener Institute for Polar and Marine Research Bremerhaven

Potsdam Summer School 15 September 2015

(2)

The tsunami simulation code TsunAWI Shallow water equations

Numerical implementation in TsunAWI Verification, limitations

The Indonesian tsunami early warning system Basic concept

The tsunami scenario database

(3)

The shallow water equations (SWE)

Phases of a tsunami

Origin in deep water at the coast

(4)

Derived from the Navier Stokes Equations

with the assumptions λH,

incompressible fluid, constant densityρ

(neglect temperatur, salinity!), Vertical velocity constant in the water column.

=⇒vertical average

(5)

The shallow water equations (SWE)

conservation of momentum

v

∂t +

pressure gradient

g∇η +

Coriolis

f k×v+

non-lin.

advection

(v·∇)v +

bottom roughness

r

H v|v| +

viscosity

∇(Kh∇v) = 0,

conservation of mass

∂η

∂t +∇ ·(Hv) = 0 with Coriolis parameterf, coefficients for bottom roughnessr and viscosityKh.

(6)

The computational domain reflects the characterics of tsunamis:

Small triangles (50m-200m) at the coast, large triangles in the deep ocean (up to 25km).

∆x ≈ min cCFL

pgH,cbathy

|∇H|

!

(7)

TsunAWI

Discretisation in space

with finite elements TriangulationT withN nodesnk ∈ N,k =1, . . . ,N

Linear conforming basis functions ϕi(x(nk)) =δik

Approximateη as linear combination ηT(x) =

N

X

i=1

ηiϕi(x)

(8)

Discretisation in space

with finite elements TriangulationT withN nodesnk ∈ N,k =1, . . . ,N

Linear conforming basis functions ϕi(x(nk)) =δik

Approximateη as linear combination ηT(x) =

N

X

i=1

ηiϕi(x)

(9)

TsunAWI

Verification: Run-up on a sloping beach

X

(10)

Verification: Run-up on a sloping beach

X

(11)

TsunAWI

Verification: Run-up on a sloping beach

For higher initial waves, the hydrostatic shallow water equations are no longer valid. Furthermore, numerical errors occur.

However, diagnostic variables like arrival time and maximum run up are still met well.

(12)

Verification: Real event, Japan 2011

Source: USGS

(13)

TsunAWI

Verification: Real event, Japan 2011

(14)

Verification: Real event, Japan 2011

(15)

TsunAWI

Verification: Real event, Japan 2011

(16)

Verification: Real event, Japan 2011

(17)

TsunAWI

Verification: Real event, Japan 2011

(18)

Verification: Real event, Japan 2011

(19)

TsunAWI

Verification: Banda Aceh 2004

Simulation shows good

agreement with measurements.

However, calibration remains difficult. The result is sensitive to

source model, Manning coefficient (bottom roughness), mesh resolution and numerical scheme, topography data.

(20)

Verification: Banda Aceh 2004

Simulation shows good

agreement with measurements.

However, calibration remains difficult. The result is sensitive to

source model, Manning coefficient (bottom roughness), mesh resolution and numerical scheme, topography data.

(21)

TsunAWI

Sensitivity study on topography data

Three groups AIFDR, ITB, AWI,

Three models ANUGA, TUNAMI-N3, TsunAWI,

Three regions Padang (Sumatra), Maumere (Flores), Palu (Sulawesi) One conclusion High quality topography data is crucial!

Free SRTM data (90m horizontal resolution,≤16m vertical accuracy) only for rough estimates,

Intermap (5m; 0.7m) and LiDar (1m; 0.15m) comparable for shallow water models,

Results more sensitive to varying data sets than to varying resolution.

(22)

Sensitivity study on topography data

Example: synthetic scenario for Maumere, Flores

(23)

Overview

The tsunami simulation code TsunAWI Shallow water equations

Numerical implementation in TsunAWI Verification, limitations

The Indonesian tsunami early warning system Basic concept

The tsunami scenario database

(24)

Warning Center

Badan Meteorologi, Klimatologi dan Geofisika, Jakarta

(25)

GITEWS System Overview

(26)

Model domain for scenarios 2011 and extension 2013

(27)

GITEWS System Overview

Earthquake magnitude and maximum amplitude

M=7.2 7.4 7.6 7.8 8.0

8.2 8.4 8.6 8.8 9.0

Mw = 23(log10M0−9.1)withM0=µdS[Nm], rigidityµ,

displacementd, area of ruptureS.

(28)

Epicenter location and maximum amplitude

M=8.0 8.0 8.0 8.0

8.0 8.0 8.0 8.0

At the coast, epicenter at large depth in rigid rock (largeµ),

(29)

Scenario data products

ETA isochrones and maximum amplitude

Example: Magnitude 9.0 in the Eastern Sunda Arc

Rakowsky et al. Tsunami Modelling Potsdam, 15.09.2015 21 / 24

(30)

Coastal forecast points

Example: Magnitude 9.0 in the Eastern Sunda Arc, zoom to Lembar, Eastern Lombok

Maximum SSH and ETA at 134.000 coastal forecast points

Time series at tide gauge

(31)

Scenario data products

Example: Small tsunami on 7 April 2010

(32)

Scenario data products

Deriving evacuation maps

e.g., Kuta, Bali

tsunami risk exposed people evacuation time

= ⇒

,local

community

evacuation map

(33)

Scenario data products

Deriving evacuation maps

e.g., Kuta, Bali

tsunami risk exposed people evacuation time

risk map (with shelters)

= ⇒

,local

community

evacuation map

(34)

Deriving evacuation maps

e.g., Kuta, Bali

tsunami risk exposed people evacuation time

= ⇒

,local

community

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