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GUIDE WAVE ANALYSIS AND FORECASTING - WMO

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5.1 Introduction<br />

National Meteorological Services in maritime countries<br />

have experienced a rapidly growing need for wave forecasts<br />

and for wave climatology. In particular the offshore<br />

oil industry needs wave data for many purposes: design<br />

sea states, fatigue analysis, operational planning and<br />

marine operations. Furthermore, consulting companies<br />

operating in the maritime sector have an increasing need<br />

for wave information in their projects.<br />

To meet this growing requirement for wave information,<br />

wave conditions must be estimated over large<br />

tracts of ocean at regular intervals, often many times a<br />

day. The volume of data and calculations makes computers<br />

indispensable. Furthermore, measured wave data<br />

are often sparse and not available when and where they<br />

are desired. Using wind information and by application<br />

of the basic physical principles that are described in<br />

Chapter 3, numerical models have been developed to<br />

make the required estimates of wave conditions.<br />

In wave modelling, we attempt to organize our<br />

theoretical and observational knowledge about waves<br />

into a form which can be of practical use to the forecaster,<br />

engineer, mariner, or the general public. The most<br />

important input to the wave models is the wind at the sea<br />

surface and the accuracy of the wave model output is<br />

strongly dependent on the quality of the input wind<br />

fields. Chapter 2 is devoted to the specification of marine<br />

winds.<br />

In the <strong>WMO</strong> Handbook on wave analysis and forecasting<br />

(1976), one particular model was described in<br />

detail to exemplify the structure and methodology of<br />

numerical wave models. Since then new classes of<br />

models have appeared and were described in the <strong>WMO</strong><br />

Guide to wave analysis and forecasting (1988). Rather<br />

than giving details of one or a few particular models, this<br />

chapter will give general descriptions of the three model<br />

classes that were defined in the SWAMP project<br />

(SWAMP Group, l985). A short description of the “third<br />

generation” WAM model developed by an international<br />

group of wave modellers is added.<br />

The basic theory of wave physics was introduced in<br />

Chapter 3. In this chapter, Section 5.2 gives a brief introduction<br />

to the basic concepts of wave modelling. Section<br />

5.3 discusses the wave energy-balance equation.<br />

Section 5.4 contains a brief description of some elements<br />

of wave modelling. Section 5.5 defines and discusses the<br />

most important aspects of the model classes. The practical<br />

applications and operational aspects of the numerical wave<br />

models are discussed in Chapter 6.<br />

CHAPTER 5<br />

INTRODUCTION TO NUMERICAL <strong>WAVE</strong> MODELLING<br />

M. Reistad with A.K. Magnusson: editors<br />

5.2 Basic concepts<br />

The mathematical description of surface waves has a<br />

large random element which requires a statistical<br />

description. The statistical parameters representing the<br />

wave field characterize conditions over a certain time<br />

period and spatial extent. Formally, over these scales, we<br />

need to assume stationarity (steadiness in time) and<br />

spatial homogeneity of the process describing the sea<br />

surface. Obviously, no such conditions will hold over the<br />

larger scales that characterize wave growth and decay.<br />

To model changing waves effectively, these scales (timestep<br />

or grid length) must be small enough to resolve the<br />

wave evolution, but it must be recognized that in time or<br />

space there are always going to be smaller scale events<br />

which have to be overlooked.<br />

The most used descriptor of the wave field is the<br />

energy-density spectrum in both frequency and direction<br />

E(f,θ), where f is the frequency, and θ the direction of<br />

propagation (see Section 1.3.7). This representation is<br />

particularly useful because we already know how to<br />

interpret what we know about wave physics in terms of<br />

the spectral components, E(f,θ). Each component can be<br />

regarded as a sinusoidal wave of which we have a<br />

reasonably well-understood theory. From this spectrum,<br />

we can deduce most of the parameters expected of an<br />

operational wave model, namely: the significant wave<br />

height, the frequency spectrum, the peak frequency and<br />

secondary frequency maxima, the directional spectrum,<br />

the primary wave direction, any secondary wave directions,<br />

the zero-crossing period, etc. (see Chapter 1).<br />

Not all models use this representation. Simpler<br />

models may be built around direct estimation of the<br />

significant wave height, or on the frequency spectrum,<br />

with directional characteristics often diagnosed directly<br />

from the wind.<br />

There is a reasonable conception of the physical<br />

processes which are thought to control wave fields. To<br />

be of general use in wave modelling, these processes are<br />

described by the response of wave ensembles, i.e. they<br />

are translated into terms of useful statistical quantities<br />

such as the wave spectrum. Not all the processes are yet<br />

fully understood and empirical results are used to varying<br />

degrees within wave models. Such representations<br />

allow a certain amount of “tuning” of wave models, i.e.<br />

model performance can be adjusted by altering empirical<br />

constants.<br />

Although models for different purposes may differ<br />

slightly, the general format is the same (see Figure 5.1<br />

for a schematic representation).

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