Changeset 3169
- Timestamp:
- Jun 16, 2006, 1:40:47 PM (19 years ago)
- Location:
- production/onslow_2006
- Files:
-
- 13 edited
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production/onslow_2006/make_gauges.py
r3159 r3169 3 3 """ 4 4 import project 5 from pylab import plot, xlabel, ylabel, title, ion, axis, savefig, close 5 from pylab import plot, xlabel, ylabel, title, ion, axis, savefig, close, text 6 6 from utilities.polygon import poly_xy 7 7 from Numeric import arange … … 54 54 xplot = [] 55 55 yplot = [] 56 names = [] 56 57 for i, point in enumerate(d): 57 58 x = point[0] … … 68 69 xplot.append(xpoint) 69 70 yplot.append(ypoint) 70 name = 'Point%d' %count 71 thisname = 'Point%d' %count 72 names.append(thisname) 71 73 count += 1 72 s = '%.2f,%.2f,%s,%.2f \n' %(xpoint,ypoint, name,0.0)74 s = '%.2f,%.2f,%s,%.2f \n' %(xpoint,ypoint,thisname,0.0) 73 75 fid.write(s) 74 76 else: … … 80 82 xplot.append(xpoint) 81 83 yplot.append(ypoint) 82 name = 'Point%d' %count 84 thisname = 'Point%d' %count 85 names.append(thisname) 83 86 count += 1 84 s = '%.2f,%.2f,%s,%.2f \n' %(xpoint,ypoint, name,0.0)87 s = '%.2f,%.2f,%s,%.2f \n' %(xpoint,ypoint,thisname,0.0) 85 88 fid.write(s) 86 89 87 90 plot(x_bound, y_bound, xplot, yplot,'b+') 91 for i, string in enumerate(names): 92 if xplot[i] > 240000 and xplot[i] < 340000: 93 text(xplot[i],yplot[i],string,fontsize=7) 88 94 89 95 axis([240000,340000, miny, maxy]) -
production/onslow_2006/make_report.py
r3136 r3169 21 21 22 22 * Introduction 23 * Modelling Methodology 23 24 * Tsunami scenario 24 25 * Inundation model … … 116 117 % * an introduction must be written in introduction.tex; a basic outline and 117 118 % some of the core inputs are already in place 119 % * outline of the modelling methodology provided in modelling_methodology.tex 118 120 % * the tsunami-genic event should be discussed in tsunami_scenario.tex 119 121 % * an computational_setup.tex file needs to be written for the particular scenario … … 165 167 \label{sec:intro} 166 168 \input{introduction} 167 169 170 \section{Modelling methodology} 171 \label{sec:methodology} 172 \input{modelling_methodology} 173 168 174 \section{Tsunami scenarios} 169 175 \label{sec:tsunamiscenario} -
production/onslow_2006/report/HAT_map.tex
r3064 r3169 1 1 \begin{figure}[hbt] 2 2 %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.jpg}} 3 \caption{Maximum inundation map for 1.5 AHD for Onslow region (in m).}3 \caption{Maximum inundation map for 1.5m AHD for Onslow region.} 4 4 \label{fig:HAT_max_inundation} 5 5 \end{figure} -
production/onslow_2006/report/LAT_map.tex
r3064 r3169 1 1 \begin{figure}[hbt] 2 2 %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.jpg}} 3 \caption{Maximum inundation map for -1.5 AHD for Onslow region (in m).}3 \caption{Maximum inundation map for -1.5m AHD for Onslow region.} 4 4 \label{fig:LAT_max_inundation} 5 5 \end{figure} -
production/onslow_2006/report/MSL_map.tex
r3064 r3169 1 1 \begin{figure}[hbt] 2 2 %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.jpg}} 3 \caption{Maximum inundation map for 0 AHD for Onslow region (in m).}3 \caption{Maximum inundation map for 0m AHD for Onslow region.} 4 4 \label{fig:MSL_max_inundation} 5 5 \end{figure} -
production/onslow_2006/report/anuga.tex
r3157 r3169 2 2 The software tool, ANUGA \cite{ON:modsim}, has been used to develop the 3 3 inundation extent 4 and associated water heightat various points in space and time.4 and associated water level at various points in space and time. 5 5 ANUGA has been developed by GA and the Australian National University 6 6 (ANU) to solve the nonlinear shallow water … … 13 13 and may change in the future. 14 14 15 The following set of information is required to undertake the tsunami15 The following set of information is required to undertake the 16 16 inundation modelling; 17 17 … … 19 19 \item onshore and offshore elevation data (topographic and bathymetric data, 20 20 see Section \ref{sec:data}) 21 \item initial condition (e.g. determined by tides)21 \item initial conditions, such as initial water levels (e.g. determined by tides) 22 22 \item boundary condition (the tsunami source as described in 23 23 Section \ref{sec:tsunamiscenario}) 24 24 \item forcing terms (such as wind) 25 \item de finition of a mesh parameter values25 \item development of numerical requirements 26 26 \end{itemize} 27 27 28 28 As part of the CRA, it was decided to provide results for the 29 ends of the tidal regimes to understand the potential impact of the 30 event. Throughout the modelling process, a number of issues became 31 evident. A standard assumption is that zero AHD is approximately 29 extremes of the tidal regimes to understand the potential range of impacts 30 from the 31 event. However, throughout the modelling process, a number of issues became 32 evident. A standard assumption is that zero Australian Height Datum 33 (AHD) is approximately 32 34 the same as Mean Sea Level (MSL). Implementing the values provided for 33 35 Highest Astronomical Tide (HAT) and Lowest Astronomical Tide (LAT) … … 35 37 Further, the recorded value for HAT will not be identical at each 36 38 point along the coastline. There 37 is e nough evidence suggesting different high tide marks (with respect39 is evidence suggesting different high tide marks (with respect 38 40 to a set datum) within 39 41 a localised region. As an aside, a current GA contract is … … 45 47 the entire study area) is not currently modelled. 46 48 In the simulations provided in this report, we assume that 47 increase of water height for the initial condition is spatially consistent ly49 increase of water height for the initial condition is spatially consistent 48 50 for the study region. 49 51 50 52 We use three initial conditions in this report; 51 -1.5 AHD, 0 AHD and 1.5 AHD. Figure \ref{fig:ic} shows the Onslow region 52 with the 1.5 AHD and -1.5 AHD contour lines shown. It is evident then 53 that much of Onslow would be inundated at 1.5 AHD. 54 53 -1.5m AHD, 0m AHD and 1.5m AHD. Figure \ref{fig:ic} shows the Onslow region 54 with the 1.5m AHD and -1.5m AHD contour lines shown. It is evident then 55 that much of Onslow would be inundated at a uniform tide at 1.5m AHD. 56 Bottom friction will generally provide resistance to the water flow 57 and thus reduce the impact somewhat. However, it is an open area 58 of research on how to determine the friction coefficients, and 59 thus it has not been incorporated 60 in the scenarios presented in this report. Therefore, the 61 results presented are over estimated to some degree. 55 62 56 63 \begin{figure}[hbt] … … 59 66 {../report_figures/contours.jpg}} 60 67 61 \caption{Onslow regions showing the 1.5 AHD and -1.5AHD contour lines.}68 \caption{Onslow regions showing the 1.5m AHD and -1.5m AHD contour lines.} 62 69 \label{fig:ic} 63 70 \end{figure} 64 71 65 72 66 It is important67 to refine the model areas to be commensurate with the underlying data especially in68 those regions where complex behaviour will occur, such as the inter-tidal69 zone and estuaries. In modelling the tsunami wave in deep water,70 it is suggested that the minimum model resolution71 be such so that there are at least72 ten cells per wavelength. The modelling73 undertaken to develop the preliminary hazard map \cite{BC:FESA}74 used a75 grid resolution which can adequately model tsunamis with a76 wavelength of 50km. Bottom friction has not been incorporated77 in the scenarios presented in this report. It78 can be accommodated in ANUGA as a forcing term, however, it is an79 open area of research on how to determine the friction coefficients.80 Therefore, the results presented are overly compensated to some degree.81 73 82 74 83 -
production/onslow_2006/report/computational_setup.tex
r3159 r3169 1 To initiate the modelling, a computationaltriangular mesh is constructed to2 cover the study region swhich has an area of around 6300 km$^2$.1 To initiate the modelling, a triangular mesh is constructed to 2 cover the study region which has an area of around 6300 km$^2$. 3 3 The cell size is chosen to balance 4 4 computational time and desired resolution in areas of interest, 5 particularly in the interface between the on and offshore. 5 particularly in the interface between the on and offshore 6 as mentioned in Section \ref{sec:}. 6 7 Figure \ref{fig:onslow_area} illustrates the data extent for the 7 8 scenario, the study area and where further mesh refinement has been made. 8 9 The choice 9 of the refinement is based around the important inter-tidal zones and 10 other important features such as islands and rivers. The most northern 11 boundary of the study area is placed approximately around the 100m contour 12 line. 10 of the refinement is based around the inter-tidal zones and 11 other important features such as islands and rivers. The northern 12 boundary of the study area is placed approximately around the 13 100m contour line. 14 15 {\bf Need some words here about why pick 100m.} 16 13 17 14 18 \begin{figure}[hbt] … … 23 27 \end{figure} 24 28 25 For the simulations, we have chosen a cell area of 500 m$^2$ per triangle 26 for the 27 region surrounding the Onslow town centre. It is worth noting here that 28 the cell 29 In addition to refining the mesh in regions where complex behaviour 30 will occur, it is important that the mesh also be 31 commensurate with the underlying data. Referring to the onshore data 32 discussed 33 in Section \ref{sec:data}, we choose a cell area 500 m$^2$ per triangle 34 for the region surrounding the Onslow town centre. 35 It is worth noting here that the cell 29 36 area will be the maximum cell area within the defined region and that each 30 cell in 31 the region does not necessarily have the same area. The cell area is increased 32 to 2500 m$^2$ for the region surrounding the coast and further increased 33 to 20000 m$^2$ for the region reaching approximately the 50m contour line. 34 The remainder of the study area has a cell area of 100000 m$^2$. 35 The resultant computational mesh is then seen in Figure \ref{fig:mesh_onslow}. 37 cell in the region does not necessarily have the same area. 38 In contrast to the onshore data, the offshore 39 data is a series of survey points which is typically not supplied on a fixed 40 grid which complicates the issue of determining an appropriate cell area. 41 In the deep water modelling such as MOST, 42 the minimum model resolution is chosen so that there at 43 least ten cells per wavelength. In developing the 44 preliminary hazard map for the Western Australia coastline, 45 \cite{BC:FESA}, a grid resolution of blah was used 46 which can adequately model tsunamis with a wavelength of 47 50km. For this scenario, the wavelength of the tsunami wave is 48 approximately 20km near the boundary indicating that a minimum 49 grid resolution of 20000m. 50 With this information, the remaining cell areas are 51 2500 m$^2$ for the region surrounding the coast, 52 20000 m$^2$ for the region reaching approximately the 50m contour line, with 53 the remainder of the study area having a cell area of 100000 m$^2$. 54 These choice of cell areas is more than adequate to propagate the tsunami wave 55 in the deepest sections of the study area\footnote{ 56 With a wavelength of 20km, the minimum (square) grid resolution would 57 be 2000m which results in a square cell area of 4000000 m$^2$. A minimum 58 triangular cell area would therefore be 2000000 m$^2$.} 59 The resultant computational mesh is shown in Figure \ref{fig:mesh_onslow}. 36 60 37 With these cell areas in place, the study area consists of 440150 triangles61 With these cell areas, the study area consists of 440150 triangles 38 62 in which water levels and momentums are tracked through time. 39 63 The associated lateral accuracy … … 42 66 that we can only be confident in the calculated inundation extent to 43 67 approximately 30m lateral accuracy within the Onslow town centre. 44 Referring to the discussion in Section \ref{sec:anuga}, it is important45 to refine the mesh to be commensurate with the underlying data especially in46 those regions where complex behaviour will occur, such as the inter-tidal47 zone and estuaries. Our choice of cell area for the region surrounding the48 Onslow town centre is commensurate with the onshore data used for this study49 (see Section \ref{sec:data}). In contrast to the onshore data, the offshore50 data is a series of survey points which is typically not supplied on a fixed51 grid which complicates the issue of determining an appropriate cell area.52 If we refer to the discussion in Section \ref{sec:data}53 on modelling a tsunami wave in deep water, we can determine an appropriate54 cell area for the deeper water. Here,55 the wavelength of the tsunami wave is approximately 20km56 near the boundary, which indicates that our cell area is more than adequate57 to propagate the tsunami wave.58 68 59 69 \begin{figure}[hbt] -
production/onslow_2006/report/damage.tex
r3079 r3169 16 16 From this database, we find that there 17 17 are 325 residential structures and a population of approximately 770 18 in Onslow 18 in Onslow\footnote{Population is determined by census data and an ABS 19 19 housing survey}. 20 20 -
production/onslow_2006/report/data.tex
r3138 r3169 47 47 by WA Department of Planning and Infrastructure. 48 48 49 The extent of the 50 data used for the tsunami impact modelling can be seen in the 51 Figure \ref{fig:onslowdataarea}. The study area covers approximately 100km 52 of coastline 53 and extends offshore to the 100m contour line and inshore to approximately 10m 54 elevation. 55 56 \begin{figure}[hbt] 57 58 \centerline{ \includegraphics[width=100mm, height=75mm] 59 {../report_figures/onslow_data_extent.png}} 60 61 \caption{Data extent for Onslow scenario. Offshore data shown in blue 62 and onshore data in green.} 63 \label{fig:onslowdataarea} 64 \end{figure} 65 49 %\begin{figure}[hbt] 50 % 51 % \centerline{ \includegraphics[width=100mm, height=75mm] 52 %{../report_figures/onslow_data_extent.png}} 53 % 54 % \caption{Data extent for Onslow scenario. Offshore data shown in blue 55 %and onshore data in green.} 56 % \label{fig:onslowdataarea} 57 %\end{figure} 66 58 67 59 Section \ref{sec:metadata} provides more details and metadata for data used for -
production/onslow_2006/report/interpretation.tex
r3156 r3169 10 10 as a function of time in the series of graphs shown in 11 11 Section \ref{sec:timeseries}. Stage is defined as the absolute 12 water height and is the water depth above the point's elevation.12 water level relative to AHD. 13 13 The graphs show these time series for 14 14 the three cases; 1.5 AHD, 0 AHD and -1.5 AHD so that comparisons can 15 15 be made. To ease these comparisons, the graphs are shown on consistent 16 scales and speeds under 0.001 m/s are not shown.16 scales. 17 17 As a useful benchmark, Table \ref{table:speedexamples} 18 18 describes typical examples for a range of velocities found in the … … 38 38 39 39 40 Examining the offshore locations, the drawdown prior to the tsunami wave 40 Examining the offshore locations shown in Section \ref{sec:timeseries}, 41 the drawdown prior to the tsunami wave 41 42 arriving at the shore can be seen to occur around 230 mins 42 43 (3.8 hours) after the tsunami is generated. -
production/onslow_2006/report/introduction.tex
r3139 r3169 1 1 2 2 This report is being provided to the Fire and Emergency Services Authority 3 (FESA) 4 as part of the Collaborative Research Agreement (CRA) 5 with Geoscience Australia. 3 (FESA) as part of the Collaborative Research Agreement (CRA) 4 with Geoscience Australia (GA). 6 5 FESA recognises the potential vulnerability of the Western Australia 7 6 coastline to tsunamigenic earthquakes originating from 8 the Sunda Arc subduction zone. There is 9 historic evidence of such events, \cite{CB:ausgeo}, 7 the Sunda Arc subduction zone that caused the December 2004 event which 8 fortunately had no impact on Australia. 9 However, there is historic evidence of tsunami events affecting the 10 Western Australia coastline, \cite{CB:ausgeo}, 10 11 and FESA has sought to assess 11 12 the relative risk of its urban and regional communities to the tsunami 12 threat and develop detailed response plans .13 threat and develop detailed response plans for a range of plausible events. 13 14 14 This report is the first in a series of studies to assess the relative 15 risk to the tsunami threat. The methods, assumptions and results of a 15 This report is the first in a series of studies assessing the relative 16 risk to the tsunami threat. Subsequent reports will not only 17 describe studies for other localities, they will also revisit these 18 scenarios as more refined hazard models become available. In this report, 19 the methods, assumptions and impacts of a 16 20 single tsunami source scenario is described for the Onslow area in the 17 21 North West shelf region. 18 22 Onslow has a population of around 800 19 is part of the Shire of Ashburton in the Pilbara region of Western Autralia 20 \footnote{http://www.pdc.wa.gov.au/region/political.htm}. Onslow supports 23 is part of the Shire of Ashburton in the Pilbara region of 24 Western Autralia\footnote{http://www.pdc.wa.gov.au/region/political.htm}. 25 Onslow supports 21 26 a variety of industries, including oil, gas, mining, cattle, 22 27 fishing and tourism. 23 28 24 29 The report will outline the methods of modelling the tsunami from its 25 source to its impact ashore. Section \ref{sec:tsunamiscenario} provides 30 source to its impact ashore and present the predicted consequences. 31 Section \ref{sec:tsunamiscenario} provides 26 32 the background to the scenario used for this study. Whilst 27 33 the return period of this scenario is unknown, it 28 can be be classed as a plausible event .34 can be be classed as a plausible event, see Section \ref{sec:tsunamiscenario}. 29 35 Future studies 30 will present a series of scenarios for a range of periods to36 will present a series of scenarios for a range of return periods to 31 37 assist FESA in developing appropriate plans for a range of event impacts. 32 The modelling technique to develop the 38 The details of the hazard modelling will not be described here, however, 39 the modelling technique to simulate the 33 40 impact ashore will be discussed in Section \ref{sec:anuga} with data inputs 34 discussed in Section \ref{sec:data}. 35 Inundation results shown in Section \ref{sec:results} and36 impact modelling results shown in Section \ref{sec:impact}.41 discussed in Section \ref{sec:data}. 42 The inundation results will be shown and discussed in Section \ref{sec:results} 43 with the impact modelling outputs shown in Section \ref{sec:impact}. 37 44 The report concludes with a summary of the results detailing issues 38 regarding data and further model development.45 regarding underlying data and further model development. 39 46 -
production/onslow_2006/report/modelling_methodology.tex
r3166 r3169 1 Tsunami hazard models have been available for a while. They generally1 Tsunami hazard models have been available some time. They generally 2 2 work by converting the energy released by a subduction earthquake into 3 3 a vertical displacement of the ocean surface. The resulting wave is 4 then propagated across a sometimes vast stretch o cean using a4 then propagated across a sometimes vast stretch of ocean using a 5 5 relatively 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. 6 resolution of two arc minutes (check this with David). 7 The maximal wave height at a fixed contour line near the coastline 8 (e.g.\ 50m) is then reported as the hazard to communities ashore. 9 Models such as Method of Splitting Tsunamies (MOST) \cite{VT:MOST} and 10 ``URS model'' \cite{xxx} follow this paradigm. 9 11 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. 12 To capture the \emph{impact} of a hydrological disaster such as tsunamis on a 13 community one must model the the details of how waves are reflected and otherwise 14 shaped by the local bathymetries as well as the dynamics of the 15 runup process onto the topography in question. 16 It is well known that local bathymetric and topographic effects are 17 critical in determining the severity of a hydrological disaster (\cite{yyy}). 18 To model the 19 details of tsunami inundation of a community one must therefore capture what is 20 known as non-linear effects and use a much higher resolution for the elevation data. 21 The model ANUGA (\cite{ON:modsim}) is suitable for this type of modelling. 22 However, using a non-linear model capable of resolving local bathymetric effects 23 and runup using detailed elevation data will require much more computational 24 resources than the typical hazard model making it infeasible to use it 25 for the entire, end-to-end, modelling. 14 26 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 27 We have adopted a hybrid approach whereby we use the output from the 28 hazard model MOST as input to ANUGA at the seaward boundary of its study area. 29 In other words, the output of MOST serves as boundary condition for the 30 ANUGA model. In this way, we restrict the computationally intensive part only to 17 31 regions where we are interested in the detailed inundation process. 18 32 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. 33 Furthermore, to avoid unnecessary computations ANUGA works with an 34 unstructured triangular mesh rather than the rectangular grids 35 used by e.g.\ MOST. The advantage of an unstructured mesh 36 is that different regions can have different resolutions allowing 37 computational resources to be directed where they are most needed. 38 For example, one might use very high resolution near a community 39 or in an estuary, whereas a coarser resolution may be sufficient 40 in deeper water where the bathymetric effects are less pronounced. 41 Figure \ref{fig:xxx} shows a mesh of variable resolution. 21 42 22 43 -
production/onslow_2006/report/tsunami_scenario.tex
r3157 r3169 3 3 \cite{BC:FESA}. In that assessment, a suite of Mw 9 earthquakes 4 4 were evenly spaced along the Sunda Arc subduction zone and there 5 was no consideration of likelihood. Other sources were not considered, such 5 was no consideration of the likelihood of each event. 6 Other sources were not considered, such 6 7 as intra-plate earthquakes near the WA coast, volcanoes, landslides 7 or asteroids. The preliminary assessment argued 8 or asteroids as they are known to be less likely. 9 The preliminary assessment argued 8 10 that the maximum magnitude of earthquakes off Java is at least 8.5 and 9 11 could potentially be as high as 9. … … 18 20 19 21 FESA are interested in the ``most frequent worst case scenario''. Whilst 20 we cannot determine what that event may be, the Mw 9 event provides22 we cannot determine exactly what that event may be, the Mw 9 event provides 21 23 a plausible worst case scenario. 22 24 23 Figure \ref{fig:mw9} shows the maximum wave height up tothe 50m contour25 Figure \ref{fig:mw9} shows the maximum wave height at the 50m contour 24 26 for a Mw 9 event off 25 27 the coast of Java. It is this event which provides the source and 26 28 boundary condition to the 27 inundation model lingpresented in this report. Description of the boundary29 inundation model presented in this report. Description of the boundary 28 30 condition particular to the Onslow study area 29 31 follows in Section \ref{sec:anuga}.
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