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Volume 1 - Main Report

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6.1.4 Physical Oceanography<br />

Two physical oceanographic survey campaigns were conducted in Deception Bay:<br />

August to September 2006 and August to September 2012. Tides and water levels,<br />

waves, flow and currents, physicochemistry and water quality were characterized for<br />

these two periods in order to describe the oceanographic conditions in Deception<br />

Bay.<br />

6.1.4.1 Tides and Water Level<br />

6.1.4.2 Waves<br />

There are few records of the water level in the Deception Bay region. The tidal<br />

characteristics established based on the water levels measured during the 2012<br />

survey campaign are used to describe the tide at the study site (Figure 6.7). The tide<br />

that enters Deception Bay is semi-diurnal, meaning that it presents two complete<br />

oscillations per day, i.e. two high waters (high tide) and two low waters (low tide).<br />

Each oscillation extends over an average period of 12 hours and 25 minutes.<br />

Tidal Characteristics<br />

Harmonic analysis of the water levels measured in 2012 (GENIVAR, 2012a) allows<br />

the establishment of a series of hourly values, which is used to establish the tidal<br />

characteristics (Table 6.8). The tidal range of 3.9 m for mean tides and 5.7 m for<br />

large tides is relatively large. The mean water level is 2.9 m and the higher high<br />

water large tide (HHWLT) is 5.8 m (Table 6.8).<br />

Storm Surge Observed in Deception Bay<br />

The analysis of the atmospheric component of the water levels measured indicates a<br />

mean variation of around 20 cm and a significant rise of the mean water level around<br />

mid-September 2012 (Figure 6.8). This rise of around 60 cm is due to the passage of<br />

a major depression. On September 13, the winds reached more than 30 km/h and<br />

the barometric pressure was below 98 kPa (Table 6.9). The combination of the<br />

passage of a depression associated with high winds and large tides causes extreme<br />

tidal events.<br />

The wave measurements taken in 2006 (Figures 6.9 and 6.10) show that the<br />

significant height (H s ) never exceeded 0.8 m. Assuming a Rayleigh distribution, it is<br />

possible to apply a conversion factor of 1.87 for H max /H s (Komar, 1998) in order to<br />

determine the maximum height of the waves. This was estimated at 1.5 m during the<br />

measuring period.<br />

Canadian Royalties Inc.<br />

GENIVAR<br />

101-53046-02 November 2012<br />

68

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