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72 ANAIS DO INSTITUTO HIDROGRÁFICO N.º 15<br />

their variation), as they are delivered instantaneously by<br />

the corresponding commands. For the case of the point,<br />

it is made a comparison with the maximum value of the<br />

respective variable in the field. It is also available the wave<br />

data evolution along the isolines. The direct connection<br />

with the pre-processing stage permits a further extension<br />

from a two-point line to a path generated by many<br />

lines as the one in figure 8 and also to define the data<br />

distribution along any isoline without imposing these as<br />

an ‘a priori’ output request to the model.<br />

4.3 Spectral analysis<br />

The harmonic or spectral analysis is a technique<br />

that unravels the waves generated by different storms<br />

and describes the complete distribution of wave energies<br />

and periods. The 1D spectrum presents variance<br />

density per unit frequency interval for each frequency.<br />

The variance units are m 2 per frequency interval<br />

Ds, which can be converted into true energy through<br />

multiplication by rg/8, where r is the water density, and<br />

g is the acceleration of gravity. The total variance for<br />

each point can be obtained by summing the variance<br />

densities. The most complete description of waves is<br />

provided by a directional wave spectrum, which includes<br />

the direction of wave approach as well as the wave variance<br />

at a specific frequency. Such a 2D spectrum is<br />

given in the three-axis plot in figure 17. As it can be seen<br />

also in the command panel of figure 17, ‘TOTAL WAVE’<br />

provides both the 1D and 2D spectra and can be followed<br />

the evolution of the spectral shape towards to the shore.<br />

Moreover could be performed comparative analyzes<br />

between the spectral shapes in various places.<br />

4.4 The surf zone conditions<br />

The processes and the phenomena associated with<br />

the depth-induced wave breaking are particularly<br />

important in the coastal engineering applications. This<br />

because a great amount of the wave energy is finally<br />

dissipated in the nearshore regions determining the<br />

geometry and composition of the beaches and influencing<br />

the coastal structures and works. A rapid and<br />

adequate evaluation of the wave conditions in these<br />

areas being therefore of essential importance. For estimating<br />

the process of wave breaking SWAN, uses the<br />

spectral version of [Eldeberky and Battjes (1996)],<br />

expanded to include directions. In terms of energy dissipation<br />

the breaking process is associated with a significant<br />

increase. Once the breaking line is identified can be<br />

evaluated the wave data along its points. In figure 18 are<br />

presented some characteristics of the breaking as the<br />

variation in relationship with the shore of the distance<br />

where is initiated the wave breaking and the distributions<br />

of the significant wave height and the depth on the<br />

breaking line. The commands available for this module<br />

could be seen also in figure 18 and they are: identifying<br />

the location of the breaking line, determining the variation<br />

of the breaking ratio along it, evaluation of the<br />

breaking type, assessing the wave direction just before<br />

breaking, computation of the number of fronts in the<br />

surf and finally displaying the dissipation variation<br />

towards to the shore. The breaker-type prediction used<br />

the deep-water form of the Iribarren number (j ‘),<br />

which combine the beach slope with the wave steepness.<br />

In reference to this parameter the breaking-type classification<br />

is the following [Komar (1998)]:<br />

Point data Line data<br />

Fig. 15 – Global data evaluation Fig. 16 – Local data assessment

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