[3064] | 1 | |
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| 2 | The software tool, ANUGA \cite{ON:modsim}, has been used to develop the |
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| 3 | inundation extent |
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[3169] | 4 | and associated water level at various points in space and time. |
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[3064] | 5 | ANUGA has been developed by GA and the Australian National University |
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| 6 | (ANU) to solve the nonlinear shallow water |
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| 7 | wave equation using the finite volume technique. |
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| 8 | An advantage of this technique is that the cell area can be changed |
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| 9 | according to areas of interest and that wetting and drying |
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| 10 | is treated robustly as part of the numerical scheme. |
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| 11 | ANUGA is continually being developed and validated. |
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| 12 | As such, the current results represent ongoing work |
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| 13 | and may change in the future. |
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| 14 | |
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[3169] | 15 | The following set of information is required to undertake the |
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[3064] | 16 | inundation modelling; |
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| 17 | |
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| 18 | \begin{itemize} |
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| 19 | \item onshore and offshore elevation data (topographic and bathymetric data, |
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| 20 | see Section \ref{sec:data}) |
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[3169] | 21 | \item initial conditions, such as initial water levels (e.g. determined by tides) |
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[3064] | 22 | \item boundary condition (the tsunami source as described in |
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[3079] | 23 | Section \ref{sec:tsunamiscenario}) |
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[3064] | 24 | \item forcing terms (such as wind) |
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[3171] | 25 | \item computational requirements relating to the mesh construction |
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[3064] | 26 | \end{itemize} |
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| 27 | |
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| 28 | As part of the CRA, it was decided to provide results for the |
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[3169] | 29 | extremes of the tidal regimes to understand the potential range of impacts |
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| 30 | from the |
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| 31 | event. However, throughout the modelling process, a number of issues became |
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| 32 | evident. A standard assumption is that zero Australian Height Datum |
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| 33 | (AHD) is approximately |
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[3136] | 34 | the same as Mean Sea Level (MSL). Implementing the values provided for |
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[3064] | 35 | Highest Astronomical Tide (HAT) and Lowest Astronomical Tide (LAT) |
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[3098] | 36 | would inundate some regions of Onslow before the simulation is even begun. |
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| 37 | Further, the recorded value for HAT will not be identical at each |
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[3064] | 38 | point along the coastline. There |
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[3169] | 39 | is evidence suggesting different high tide marks (with respect |
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[3064] | 40 | to a set datum) within |
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[3136] | 41 | a localised region. As an aside, a current GA contract is |
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[3064] | 42 | extracting information from LANDSAT imagery to reconstruct the |
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| 43 | tidal variations for various WA locations. Future modelling of |
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| 44 | these areas will incorporate this information. |
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| 45 | Further, the dynamics of |
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| 46 | tidal effects (that is, the changes in water height over time for |
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| 47 | the entire study area) is not currently modelled. |
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| 48 | In the simulations provided in this report, we assume that |
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[3169] | 49 | increase of water height for the initial condition is spatially consistent |
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[3098] | 50 | for the study region. |
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[3064] | 51 | |
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| 52 | We use three initial conditions in this report; |
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[3169] | 53 | -1.5m AHD, 0m AHD and 1.5m AHD. Figure \ref{fig:ic} shows the Onslow region |
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| 54 | with the 1.5m AHD and -1.5m AHD contour lines shown. It is evident then |
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| 55 | that much of Onslow would be inundated at a uniform tide at 1.5m AHD. |
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| 56 | Bottom friction will generally provide resistance to the water flow |
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| 57 | and thus reduce the impact somewhat. However, it is an open area |
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| 58 | of research on how to determine the friction coefficients, and |
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| 59 | thus it has not been incorporated |
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| 60 | in the scenarios presented in this report. Therefore, the |
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| 61 | results presented are over estimated to some degree. |
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[3064] | 62 | |
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| 63 | \begin{figure}[hbt] |
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| 64 | |
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[3078] | 65 | \centerline{ \includegraphics[width=150mm, height=100mm] |
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| 66 | {../report_figures/contours.jpg}} |
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[3064] | 67 | |
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[3169] | 68 | \caption{Onslow regions showing the 1.5m AHD and -1.5m AHD contour lines.} |
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[3064] | 69 | \label{fig:ic} |
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| 70 | \end{figure} |
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| 71 | |
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[3157] | 72 | |
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[3064] | 73 | |
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[3098] | 74 | |
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