1 | %\clearpage |
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2 | The following subsections detail the time series at the locations |
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3 | described in the previous table |
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4 | %table \ref{table:gaugelocations} |
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5 | for Highest Astronomical Tide (HAT), Lowest Astronomical Tide (LAT) and |
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6 | Mean Sea Level (MSL) conditions. These locations |
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7 | have been chosen to assist in describing the features of the tsunami wave |
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8 | and the resultant impact ashore. Here, we assume that MSL coincides with |
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9 | AHD zero. This is a standard assumption and confirmed with the WA DPI. |
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10 | The graph ranges for both stage and |
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11 | velocity are made consistent for each of comparison. In addition, velocities |
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12 | under 0.001 m/s are not shown. As a useful benchmark, the following table |
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13 | describes typical examples for a range of velocities found in the |
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14 | simulations. |
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15 | |
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16 | \begin{table} |
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17 | \label{table:speed_examples} |
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18 | \caption{Examples of a range of velocities.} |
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19 | \begin{center} |
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20 | \begin{tabular}{|l|l|}\hline |
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21 | Velocity (m/s) & Example \\ \hline |
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22 | 1 & leisurely stroll pace\\ \hline |
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23 | 1.5 & average walking pace \\ \hline |
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24 | 2 & 100m Olympic male freestyle \\ \hline |
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25 | 3 & mackeral \\ \hline |
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26 | 4 & average person maintain for 1000m \\ \hline |
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27 | 5 & blue whale \\ \hline |
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28 | 10 & 100m Olympic male sprinter \\ \hline |
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29 | 16 & car travelling in urban zones (60 km/hr) \\ \hline |
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30 | \end{tabular} |
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31 | \end{center} |
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32 | \end{table} |
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33 | |
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34 | In simulating different tidal conditions, we assume that the |
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35 | tidal conditions are the same for all locations in the study region. |
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36 | It is worth noting here that ANUGA does not model tidal effects (that is, |
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37 | the change in water height over time). To incorporate this effect in |
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38 | a consistent way would also involve having information about the |
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39 | difference in tide heights for every location in the region. This |
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40 | information is not available on a national scale, |
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41 | therefore our approach of applying a uniform change in water |
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42 | height is a reasonable one. |
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43 | |
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44 | The Australian Hydrographic Office fair sheet for Onslow describes the |
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45 | chart datum to be LAT with MSL and HAT being 1.5 and 3 respectively. This |
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46 | then places HAT and LAT at 1.5 AHD and -1.5 AHD respectively. Other |
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47 | detail on the chart describes the blah de blah mark to be MHWS. |
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48 | |
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49 | Hamish/Kathryn - does the Onslow coastline coincide with the yellow bit on the |
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50 | Onslow map? If so, does that place AHD 0 at MHWS? |
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51 | |
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52 | It is evident from figure \ref{fig:ic_high} |
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53 | that much of Onslow would be inundated at Highest Astronomical Tide (HAT) |
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54 | (1.5m above MSL). |
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55 | HAT is the projected tide on a 19 year cycle (occurring when a number of |
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56 | astronomical conditions happen simultaneously), and Mean High Water Springs |
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57 | (MHWS) is the tide which is projected to occur ... (get the words |
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58 | from the ANTT 06). The |
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59 | Australian National Tidal Tables 2006 determines MHWS for Onslow to be 1m |
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60 | (adjusted to AHD) which also places regions within the study area under |
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61 | water before a tsunami wave reaches the shore. Using HAT or even |
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62 | MHWS in this way has significant infrastructure inundated which does not |
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63 | seem reasonable. Therefore, we show results for MSL only and |
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64 | provide a |
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65 | qualitative discussion on the changes to the inundation at HAT and LAT. |
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66 | |
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67 | \begin{figure}[hbt] |
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68 | |
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69 | %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.png}} |
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70 | |
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71 | \caption{Initial condition for mean sea level.} |
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72 | \label{fig:ic_zero} |
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73 | \end{figure} |
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74 | |
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75 | \begin{figure}[hbt] |
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76 | |
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77 | %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.png}} |
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78 | |
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79 | \caption{Initial condition for lowest astronomical tide.} |
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80 | \label{fig:ic_low} |
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81 | \end{figure} |
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82 | |
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83 | \begin{figure}[hbt] |
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84 | |
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85 | %\centerline{ \includegraphics[width=100mm, height=75mm]{../report_figures/.png}} |
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86 | |
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87 | \caption{Initial condition for highest astronomical tide.} |
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88 | \label{fig:ic_high} |
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89 | \end{figure} |
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90 | |
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91 | Examining the offshore gauges, the drawdown prior to the tsunami wave |
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92 | arriving at the shore can be seen to occur around 230 mins |
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93 | (3.8 hours) after the tsunami is generated. |
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94 | Prior to the drawdown, maximum amplitudes are approximately 50cm at |
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95 | West of Groyne and the mouth of Beadon Creek, for example. The first wave |
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96 | after the drawdown ranges from approximatly 2m in the |
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97 | west of Beadon Bay to 1.5m in the east of Beadon Bay. The velocity |
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98 | sharply increases at drawdown with further increases as the |
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99 | wave grows in amplitude. |
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100 | There is an increased amplitude of approximately 3m found in |
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101 | east of Beadon Bay for the secondary wave, as opposed to the first wave. |
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102 | This feature is also evident at the West of Groyne location. |
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103 | This may be due to the geography of the bay, including the groyne west of |
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104 | the creek mouth opening, the local bathymetry |
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105 | and the direction of the tsunami wave. |
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106 | |
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107 | The maximum velocity found for the offshore gauges occurs at the West of |
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108 | Groyne location with velocities halved at the Beadon Bay west location. |
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109 | The Beadon Bay west velocity is greater that the gauge in the east of Beadon |
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110 | Bay. There is similar differences in amplitude (from drawdown to maximum |
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111 | amplitude), however, the west gauge is in deeper water than the east |
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112 | gauge which may indicate the increased velocity found in the east of the |
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113 | bay. |
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114 | |
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115 | Subsequent drawdowns are seen as the multitude of waves which make up the |
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116 | event propagate towards the shore. |
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117 | |
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118 | %At some gauge locations, these |
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119 | %subsequent waves cause significantly increased inundation than that of |
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120 | %the first wave. This is particularly seen at the Beadon Creek Docks, |
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121 | %West of Groyne and Beadon Creek locations. |
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122 | |
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123 | ({\bf Note, these words are assuming that the current simulations are OK, |
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124 | and will have to be updated once we have more information about |
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125 | the tides etc}). |
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126 | It is evident for each simulation that the sand dunes west of |
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127 | Onslow are very effective in halting the tsunami wave. The height of these |
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128 | sand dunes are approximately 10m which is more than enough to halt |
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129 | the largest of the tsunami waves which occurs for the |
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130 | high tide simulation. There is inundation between the sand dunes at high |
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131 | tide, however, this water penetrated from the north east (via |
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132 | Onslow town cetnre) rather than seaward. |
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133 | The same feature is evident for the sand dunes east of Onslow which |
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134 | rise to 15m in height. Currently, ANUGA can not model changes |
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135 | to the bathymetry or topography due to effects of the water flow. |
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136 | Therefore, we do not know whether these sand dunes would withstand the |
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137 | transmitted energy of the tsunami wave. |
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138 | |
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139 | The wave penetrates the river east of Onslow with increasingly |
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140 | greater inundation as the tide changes from LAT to HAT. |
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141 | |
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142 | As expected, there is greater inundation at high tide. The major road |
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143 | into Onslow, the Onslow Mount Stuart Rd, remains free of inundation for |
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144 | all tidal scenarios. Beadon Creek Rd which services the wharf in the |
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145 | river becomes increasingly inundated as the tide rises. Only the |
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146 | entry to the wharf on Beadon Creek Rd is sufficiently inundated at LAT |
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147 | to stop traffic. At HAT however, essentially the entire road |
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148 | would be impassable. |
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149 | |
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150 | There is significant inundation of at |
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151 | least 2m on the foreshore of Onslow for MSL and HAT. |
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152 | The inundation extent increases as the tide rises, pushing the edges |
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153 | of the majority of the road infrastructure in the Onslow town centre. |
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