Sea state : interpret wave patterns

In Weather4D, as generally in other applications, sea ​​state forecasts are described by ocean models. The most used is the model WW3 (Wave Watch III), published by FNMOC (Fleet Numerical Meteorology and Oceanography Center) of the US Navy, with a global model due to 7 days and resolution 1° (60NM), and a Europe model to 3 days and resolution 0.2° (12NM). Météo-France publish the models MFAUM (Wave Assimilated Model) coupled with the ARPEGE and AROME weather models with three resolutions : Global at 0.5° (30NM), Europe at 0.1° (6NM), France at 0.025° (1,5NM) with variable deadlines (¹).

Each of these models provides three essential data for navigation (among several dozen other oceanographic data) : the height, the direction and period waves. This is the “sea of ​​wind” from associated weather models.

However, these three data raise some questions : what relationship between height and period, can we predict if the waves break, what reliability when approaching the coast ? Let's try to answer it (²) …

Les données affichées dans Weather4D sur le météogramme et par champs de couleurs (isoplages par pas de 0,50m).

Data displayed in Weather4D on the meteogram and by color fields (isolations in steps of 0.50m).

Wave propagation medium

We must first distinguish two wave propagation environments. : in deep water (dispersive environment) and shallow water (non-dispersive environment). Only the deep sea environment will be discussed here, far from the coasts and the rise of the seabed.

We determine the notion of dispersive environment by a ratio between the wavelength of the waves (The) and the depth of the sea (P). Without going into mathematical details, to simplify the propagation in deep water we consider, i.e. where the waves are not affected by the bottom, when P > L/2 or L<2P, which amounts to the same. For example, with a wavelength of 150m, the depth must be greater than 75m. With a sounding at 60m, the wavelength must not exceed 120m.

Wave characteristics

The Period (T) is the time interval between two crests, or two hollows, expressed in seconds. In deep water, the Wavelength (The) expressed in meters is equal to 1,5T². Example : waves of 8 period seconds will have a wavelength of 1.5×8² = 96m (≅ 100m). The Velocity, or speed of propagation, is equal to 1,5T expressed in meters per second. In the example, 1,5×8 = 12 m/s (23 knots). The Height is the vertical distance from the crest to the hollow, expressed in meters.

The values ​​of these data are closely related to the wind force, to the expanse over which the wind blows, called generating area, and the distance over which the wind is blowing without encountering an obstacle, called the fetch.

La distance sans obstacle sur laquelle s'exerce le vent

The unobstructed distance over which the wind is blowing

Wave trains

The state of the sea is often made up of the superposition of several wave systems.. Groups are formed by the combination of wave trains of the same height and direction, but having slightly different periods. The waves will thus move in groups whose speed in deep water will be approximately half the speed of each isolated wave.. The speed of the group is therefore calculated V = C/2, i.e. V = 1.5T/2 = 0,75T. Example : the speed of a group of waves whose period is 8 seconds will be 1.5×8/2 = 6m/s (12 knots). We therefore observe cyclically groups of steeper waves, the heights being added, and significantly lower wave intervals.

Les groupes de vagues se forment par le décalage des périodes qui crée des juxtapositions cycliques

Wave groups are formed by the shift of periods which creates cyclical juxtapositions (²)

The surge

The breaking of a wave is determined by the notion of Camber (γ). This data is defined by the formula γ=H/L, or the ratio of wave height to wavelength. We demonstrate by calculation that the wave breaks, in deep water, when the camber γ>0,14. This limit value can be reached, either by the force of the wind alone, either by the wind against a strong current (in the Channel, in example, when the tide turns against the wind), by the crossing of wave trains of different directions, or by a rising sea floor (in the latter case we enter a non-dispersive environment).

Example with waves of H=5m and T=6s, limited breaking risk :

      • L = 1,5T² = 1,5×6² = 54m
      • γ = H/L = 5/54 = 0,09

We can easily calculate, for each wave height, the limit period giving a camber γ>0,14. Here are some examples :

Height Calculated period Rounded period
5meters 4,88s. 5s.
6meters 5,35s. 5,5s.
8meters 6,2s. 6,5s.
10meters 6,9s. 7s.

But be careful, we must not confuse “breaking wave” and “breaking crest” which occurs much earlier, from 30-35 knots of wind, when gusts sweep over the tops of waves as in the illustration below. On the other hand, in the wave groups mentioned previously, at the same period, groups of steeper waves can reach heights causing a limit camber.

Crêtes déferlantes sous une Tramontane à 40 nds établis, à l'approche du Cap Sicié.

Breaking crests under a Tramontane at 40 nds established, approaching Cape Sicié.

As you approach the coast, things get complicated. Wave calculations in a non-dispersive environment, therefore at shallow depth, become more complex and are the subject of numerous specialist literature, to which I do not belong. Each of us knows perfectly well that the rise of the continental shelf causes a significant worsening of the state of the sea during strong westerly winds., even more on the Channel when the tide is against, and that the Tramontana can form a breaking swell on the northern coasts of the Balearic Islands, as in the following illustration.

La mer de L=100m va lever sur la ligne de sonde 50m au nord de Minorque et déferler à la côte.

The sea of ​​L = 100m will rise on the sounding line 50m north of Menorca and break to the coast.

Such a situation makes surfers happy !

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(¹) See, for more details, the User manuals of Weather4D to download for free.
(²) Source : General and Maritime Meteorology, Météo-France – 2001
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