Page 44 - Marine Structural Design
P. 44

Chapter 2 Wave Loads for Ship Design and Classijication                21


                  The parameters used to describe ocean waves are stochastic processes, which are continuous
                  functions of time. Thus the measurements of the same parameter taken at different times could
                  result in very dissimilar readings. The data regarding the parameters used to describe ocean
                  waves, is collected by taking different samples over a period of time. For the validity of this
                  data, it is essential to ensure that each sample is collected under similar conditions. In the case
                  of ocean waves,  a parameter such as sea elevation is influenced by  a number of  different
                  variables, such as wind speed and wind direction. In order to be certain that these different
                  variables remain relatively constant from sample to sample, the data is collected within a short
                  observation period.
                  A random process is stationary if the statistical characteristics of the process do not change
                  with time t. This means that the averages and moments of the stationary process are invariant
                  over time. Ocean data is usually collected from samples spanning anywhere from 30 minutes
                  to 3 hours, because during this period the data is considered stationary.
                  There are two different methods for defining averages of samples of a random process: the
                  ensemble and the temporal. The ensemble average is the average taken over all of the samples
                  at one instant in time. The temporal average is the average of a particular sample over time. In
                  the case of random processes such as ocean waves, the time averages formed from a single
                  sample over a given time interval are equal to the ensemble averages. This situation is known
                  as an ergodic random process.
                  A random process may be characterized as a narrow-band or a wide-band process. In simple
                  terms, a narrow-band process is made up of waves with frequencies lying within a narrow
                  range, while a wide-band process consists of waves with widely varying frequencies. Ocean
                  wave data shows that  a  fully developed, wind-generated, mid-ocean sea-state (Le.  with  no
                  growth or decay, and no coastal effects), is essentially narrow-banded. Of course, there are
                  always wave components, which differ by having a high frequency, but these waves tend to be
                  small in both height and length and have little effect on the ship. It is also interesting to note
                  that a ship acts as a filter, only a narrow band of wave frequencies has an effect on the ship's
                  motion and hull girder loads. Thus the ship's response is even more narrow-banded than the
                  sea itself and this response is usually also characterized as a Gaussian and stationary process
                 just like the ocean waves.
                  Chapter 24 of this book contains more information on random variable definitions.
                  2.2.2   Statistical Representation of the Sea Surface

                  This Section deals with the representation of a complete sea surface. Of course, we know that
                 the sea surface is highly irregular and random under all sorts of conditions, calm or stormy
                 weather. However, it has been found that this random process may be accurately represented
                 by a series of different regular waves of varying heights, lengths, directions and phase that all
                 superimposed on each other.
                 Three papers, which paved the way for further work on statistical representations of the sea
                  surface,  were  published  by  Pierson  (1952),  St.  Denis  and  Pierson  (1953),  and  Pierson,
                 Neumann, and James (1955). These papers proved that the sea surface could be represented by
                 the superposition of a large number of regular sinusoidal waves of varying frequencies. A
                 typical sinusoidal wave may be represented by the following:
                      &,t)  = asin(-   lo^ - o + 8)                                    (2.3)
                                        t
                 where,
   39   40   41   42   43   44   45   46   47   48   49