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62 Fundamentals of Ocean Renewable Energy































            FIG. 3.15  Water surface elevation time series at two contrasting locations: Boston (semidiurnal)
            and Mississippi Sound (diurnal). (Data from NOAA.)



                                         H K1 + H O1
                                     F =                               (3.20)
                                         H M2 + H S2
            where H M2 , etc. is the amplitude of the M2 tidal constituent, etc. F can be
            used to quantify the type of tide, using the interpretation shown in Table 3.2.
            Form factor is plotted globally from the FES2012 global tidal atlas in Fig. 3.16.
            Although the majority of high tidal stream regions throughout the world are
            semidiurnal (e.g. the northwest European shelf seas or the northeast of the
            United States), many important regions are diurnal, such as the South China
            Sea, East China Sea, New Guinea, and Northern Australia. It is therefore
            important that semidiurnal and diurnal constituents be included in any resource
            assessment.


            3.10 OVERTIDES AND TIDAL ASYMMETRY
            As described in previous sections, astronomical tides are generated by the
            gravitational forces of the Sun and the Moon on the oceans; therefore, the
            frequencies of tidal signals (water elevation and velocity) can be directly related
            to lunar or solar days in the deep oceans. The propagation of barotropic tides
            in the deep ocean can be assumed to be mainly governed by linear processes.
            The interaction of tidal components in the deep ocean leads to subharmonic
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