GUIDE WAVE ANALYSIS AND FORECASTING - WMO
GUIDE WAVE ANALYSIS AND FORECASTING - WMO
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).