source: production/pt_hedland_2006/report/interpretation.tex @ 3340

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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 Pt Hedland describes the
45chart datum to be -4.132m below berth 3 with HAT, MHWS, MSL and LAT
46placed at 7.5m, 6.8m  4.1 and 3.9m respecitively above the chart datum.
47Assuming MSL is equivalent to AHD 0, then
48HAT and LAT are 3.37 AHD and -0.23 AHD respectively.
49Other detail on the chart describes the blah de blah mark to be MHWS.
50
51It is evident from figure \ref{fig:ic_high} 
52that much of Pt Hedland would be inundated at Highest Astronomical Tide (HAT)
53(3.37m above MSL).
54HAT is the projected tide on a 19 year cycle (occurring when a number of
55astronomical conditions happen simultaneously), and Mean High Water Springs
56(MHWS) is the tide which is projected to occur ... (get the words
57from the ANTT 06). The
58Australian National Tidal Tables 2006 determines MHWS for Pt Hedland to be
592.67m (adjusted to AHD) which also places regions within the study area under
60water before a tsunami wave reaches the shore. Using HAT or even
61MHWS in this way has significant infrastructure inundated which does not
62seem reasonable. Therefore, we show results for MSL only and
63provide a
64qualitative discussion on the changes to the inundation at HAT and LAT. 
65
66\begin{figure}[hbt]
67
68  %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.png}}
69
70  \caption{Initial condition for mean sea level.}
71  \label{fig:ic_zero}
72\end{figure}
73
74\begin{figure}[hbt]
75
76  %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.png}}
77
78  \caption{Initial condition for lowest astronomical tide.}
79  \label{fig:ic_low}
80\end{figure}
81
82\begin{figure}[hbt]
83
84  %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.png}}
85
86  \caption{Initial condition for highest astronomical tide.}
87  \label{fig:ic_high}
88\end{figure}
89
90Examining the offshore gauges, the drawdown prior to the tsunami wave
91arriving at the shore can be seen to occur around 230 mins 
92(3.8 hours) after the tsunami is generated.
93Prior to the drawdown, maximum amplitudes are approximately ? at
94? and the ?, for example. The first wave
95after the drawdown ranges from approximatly ?m in the
96? to ?m in the ?. The velocity
97sharply increases at drawdown with further increases as the
98wave grows in amplitude.
99There is an increased amplitude of approximately 3m found in
100east of Beadon Bay for the secondary wave, as opposed to the first wave.
101This feature is also evident at the West of Groyne location.
102This may be due to the geography of the bay, including the groyne west of
103the creek mouth opening, the local bathymetry
104and the direction of the tsunami wave.
105
106The maximum velocity found for the offshore gauges occurs at the West of
107Groyne location with velocities halved at the Beadon Bay west location.
108The Beadon Bay west velocity is greater that the gauge in the east of Beadon
109Bay. There is similar differences in amplitude (from drawdown to maximum
110amplitude), however, the west gauge is in deeper water than the east
111gauge which may indicate the increased velocity found in the east of the
112bay. 
113
114Subsequent drawdowns are seen as the multitude of waves which make up the
115event propagate towards the shore.
116
117%At some gauge locations, these
118%subsequent waves cause significantly increased inundation than that of
119%the first wave. This is particularly seen at the Beadon Creek Docks,
120%West of Groyne and Beadon Creek locations.
121
122As expected, there is greater inundation at high tide. The major road
123into Onslow, the Onslow Mount Stuart Rd, remains free of inundation for
124all tidal scenarios. Beadon Creek Rd which services the wharf in the
125river becomes increasingly inundated as the tide rises. Only the
126entry to the wharf on Beadon Creek Rd is sufficiently inundated at LAT
127to stop traffic. At HAT however, essentially the entire road
128would be impassable.
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