source: production/onslow_2006/report/interpretation.tex @ 3005

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1%\clearpage
2The following subsections detail the time series at the locations
3described in the previous table
4%table \ref{table:gaugelocations}
5for Highest Astronomical Tide (HAT), Lowest Astronomical Tide (LAT) and
6Mean Sea Level (MSL) conditions. These locations
7have been chosen to assist in describing the features of the tsunami wave
8and the resultant impact ashore. Here, we assume that MSL coincides with
9AHD zero. This is a standard assumption and confirmed with the WA DPI.
10The graph ranges for both stage and
11velocity are made consistent for each of comparison. In addition, velocities
12under 0.001 m/s are not shown. As a useful benchmark, the following table
13describes typical examples for a range of velocities found in the
14simulations.
15
16\begin{table}
17\label{table:speed_examples}
18\caption{Examples of a range of velocities.}
19\begin{center}
20\begin{tabular}{|l|l|}\hline
21Velocity (m/s) & Example \\ \hline
221 & leisurely stroll pace\\ \hline
231.5 & average walking pace \\ \hline
242 & 100m Olympic male freestyle \\ \hline
253 & mackeral \\ \hline
264 & average person maintain for 1000m \\ \hline
275 & blue whale \\ \hline
2810 & 100m Olympic male sprinter \\ \hline
2916 & car travelling in urban zones (60 km/hr) \\ \hline
30\end{tabular}
31\end{center}
32\end{table}
33
34In simulating different tidal conditions, we assume that the
35tidal conditions are the same for all locations in the study region.
36It is worth noting here that ANUGA does not model tidal effects (that is,
37the change in water height over time). To incorporate this effect in
38a consistent way would also involve having information about the
39difference in tide heights for every location in the region. This
40information is not available on a national scale,
41therefore our approach of applying a uniform change in water
42height is a reasonable one.
43
44The Australian Hydrographic Office fair sheet for Onslow describes the
45chart datum to be LAT with MSL and HAT being 1.5 and 3 respectively. This
46then places HAT and LAT at 1.5 AHD and -1.5 AHD respectively. Other
47detail on the chart describes the blah de blah mark to be MHWS.
48
49Hamish/Kathryn - does the Onslow coastline coincide with the yellow bit on the
50Onslow map? If so, does that place AHD 0 at MHWS?
51
52It is evident from figure \ref{fig:ic_high} 
53that much of Onslow would be inundated at Highest Astronomical Tide (HAT)
54(1.5m above MSL).
55HAT is the projected tide on a 19 year cycle (occurring when a number of
56astronomical conditions happen simultaneously), and Mean High Water Springs
57(MHWS) is the tide which is projected to occur ... (get the words
58from the ANTT 06). The
59Australian National Tidal Tables 2006 determines MHWS for Onslow to be 1m
60(adjusted to AHD) which also places regions within the study area under
61water before a tsunami wave reaches the shore. Using HAT or even
62MHWS in this way has significant infrastructure inundated which does not
63seem reasonable. Therefore, we show results for MSL only and
64provide a
65qualitative discussion on the changes to the inundation at HAT and LAT. 
66
67\begin{figure}[hbt]
68
69  %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.png}}
70
71  \caption{Initial condition for mean sea level.}
72  \label{fig:ic_zero}
73\end{figure}
74
75\begin{figure}[hbt]
76
77  %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.png}}
78
79  \caption{Initial condition for lowest astronomical tide.}
80  \label{fig:ic_low}
81\end{figure}
82
83\begin{figure}[hbt]
84
85  %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.png}}
86
87  \caption{Initial condition for highest astronomical tide.}
88  \label{fig:ic_high}
89\end{figure}
90
91Examining the offshore gauges, the drawdown prior to the tsunami wave
92arriving at the shore can be seen to occur around 230 mins 
93(3.8 hours) after the tsunami is generated.
94Prior to the drawdown, maximum amplitudes are approximately 50cm at
95West of Groyne and the mouth of Beadon Creek, for example. The first wave
96after the drawdown ranges from approximatly 2m in the
97west of Beadon Bay to 1.5m in the east of Beadon Bay. The velocity
98sharply increases at drawdown with further increases as the
99wave grows in amplitude.
100There is an increased amplitude of approximately 3m found in
101east of Beadon Bay for the secondary wave, as opposed to the first wave.
102This feature is also evident at the West of Groyne location.
103This may be due to the geography of the bay, including the groyne west of
104the creek mouth opening, the local bathymetry
105and the direction of the tsunami wave.
106
107The maximum velocity found for the offshore gauges occurs at the West of
108Groyne location with velocities halved at the Beadon Bay west location.
109The Beadon Bay west velocity is greater that the gauge in the east of Beadon
110Bay. There is similar differences in amplitude (from drawdown to maximum
111amplitude), however, the west gauge is in deeper water than the east
112gauge which may indicate the increased velocity found in the east of the
113bay. 
114
115Subsequent drawdowns are seen as the multitude of waves which make up the
116event propagate towards the shore.
117
118%At some gauge locations, these
119%subsequent waves cause significantly increased inundation than that of
120%the first wave. This is particularly seen at the Beadon Creek Docks,
121%West of Groyne and Beadon Creek locations.
122
123({\bf Note, these words are assuming that the current simulations are OK,
124and will have to be updated once we have more information about
125the tides etc}).
126It is evident for each simulation that the sand dunes west of
127Onslow are very effective in halting the tsunami wave. The height of these
128sand dunes are approximately 10m which is more than enough to halt
129the largest of the tsunami waves which occurs for the
130high tide simulation. There is inundation between the sand dunes at high
131tide, however, this water penetrated from the north east (via
132Onslow town cetnre) rather than seaward.
133The same feature is evident for the sand dunes east of Onslow which
134rise to 15m in height. Currently, ANUGA can not model changes
135to the bathymetry or topography due to effects of the water flow.
136Therefore, we do not know whether these sand dunes would withstand the
137transmitted energy of the tsunami wave.
138
139The wave penetrates the river east of Onslow with increasingly
140greater inundation as the tide changes from LAT to HAT.
141
142As expected, there is greater inundation at high tide. The major road
143into Onslow, the Onslow Mount Stuart Rd, remains free of inundation for
144all tidal scenarios. Beadon Creek Rd which services the wharf in the
145river becomes increasingly inundated as the tide rises. Only the
146entry to the wharf on Beadon Creek Rd is sufficiently inundated at LAT
147to stop traffic. At HAT however, essentially the entire road
148would be impassable.
149
150There is significant inundation of at
151least 2m on the foreshore of Onslow for MSL and HAT.
152The inundation extent increases as the tide rises, pushing the edges
153of the majority of the road infrastructure in the Onslow town centre.
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