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Timestamp:
Jun 16, 2006, 1:40:47 PM (19 years ago)
Author:
sexton
Message:

updates to Onslow report

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  • production/onslow_2006/report/modelling_methodology.tex

    r3166 r3169  
    1 Tsunami hazard models have been available for a while. They generally
     1Tsunami hazard models have been available some time. They generally
    22work by converting the energy released by a subduction earthquake into
    33a vertical displacement of the ocean surface. The resulting wave is
    4 then propagated across a sometimes vast stretch ocean using a
     4then propagated across a sometimes vast stretch of ocean using a
    55relatively coarse model based on bathymetries with a typical
    6 resolution of 2 arc minutes (check this with David). Near a coastline the maximal wave height at a fixed contour line (e.g.\ 50m) is then reported as the
    7 hazard to communities ashore.
    8 Models such as Method of Splitting Tsunamies (MOST) \cite{VT:MOST} and ``URS model'' \cite{person:urs} follow this paradigm.
     6resolution of two arc minutes (check this with David).
     7The maximal wave height at a fixed contour line near the coastline
     8(e.g.\ 50m) is then reported as the hazard to communities ashore.
     9Models such as Method of Splitting Tsunamies (MOST) \cite{VT:MOST} and
     10``URS model'' \cite{xxx} follow this paradigm.
    911
    10 To capture the \emph{impact} of a hydrological disaster such as tsunamies on a community one must model the the details of how waves are reflected and otherwise shaped by the local bathymetries as well as the dynamics of the runup process onto the topography in question.
    11 It is well known that local bathymetric and topographic effects are critical in determining the severity of a hydrological disaster (\cite{yyy}). To model the
    12 details of tsunami inundation of a community one must therefore capture what is known as non-linear effects and use a much higher resolution for the elevation data. The model ANUGA (\cite{ON:modsim}) is suitable for this type of modelling.
    13 However, using a non-linear model capable of resolving local bathymetric effects and runup using detailed elevation data will require much more computational resources than the typical hazard model making it infeasible to use it for the entire, end-to-end, modelling.
     12To capture the \emph{impact} of a hydrological disaster such as tsunamis on a
     13community one must model the the details of how waves are reflected and otherwise
     14shaped by the local bathymetries as well as the dynamics of the
     15runup process onto the topography in question.
     16It is well known that local bathymetric and topographic effects are
     17critical in determining the severity of a hydrological disaster (\cite{yyy}).
     18To model the
     19details of tsunami inundation of a community one must therefore capture what is
     20known as non-linear effects and use a much higher resolution for the elevation data.
     21The model ANUGA (\cite{ON:modsim}) is suitable for this type of modelling.
     22However, using a non-linear model capable of resolving local bathymetric effects
     23and runup using detailed elevation data will require much more computational
     24resources than the typical hazard model making it infeasible to use it
     25for the entire, end-to-end, modelling.
    1426
    15 We have adopted a hybrid approach whereby we use the output from the the
    16 hazard model MOST as input to ANUGA at the seaward boundary of its study area. In other words, the output of MOST serves as boundary condition for the ANUGA model. In this way, we restrict the computationally intensive part only to
     27We have adopted a hybrid approach whereby we use the output from the 
     28hazard model MOST as input to ANUGA at the seaward boundary of its study area.
     29In other words, the output of MOST serves as boundary condition for the
     30ANUGA model. In this way, we restrict the computationally intensive part only to
    1731regions where we are interested in the detailed inundation process. 
    1832
    19 Furthermore, to avoid unnecessary computations ANUGA works with an unstructured triangular mesh rather than the rectangular grids used by e.g.\ MOST. The advantage of an unstructured mesh is that different regions can have different resolutions allowing computational resources to be directed where they are needed the most. For example, one might use very high resolution near a community or in an estuary whereas a coarser resolution may be sufficient in deeper water where the bathymetric effects are less pronounced. Figure \ref{fig:xxx} shows a mesh of
    20 variable resolution.
     33Furthermore, to avoid unnecessary computations ANUGA works with an
     34unstructured triangular mesh rather than the rectangular grids
     35used by e.g.\ MOST. The advantage of an unstructured mesh
     36is that different regions can have different resolutions allowing
     37computational resources to be directed where they are most needed.
     38For example, one might use very high resolution near a community
     39or in an estuary, whereas a coarser resolution may be sufficient
     40in deeper water where the bathymetric effects are less pronounced.
     41Figure \ref{fig:xxx} shows a mesh of variable resolution.
    2142
    2243
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