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Practical Ship Hydrodynamics

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134 <strong>Practical</strong> <strong>Ship</strong> <strong>Hydrodynamics</strong><br />

The average frequency (occurrences/time) of upward zero crossings and also<br />

as the above definition of amplitudes of r is derived from the r spectrum to:<br />

�<br />

� 1 � 2<br />

ω2 eSr⊲ω, ⊳ d dω<br />

f0 D 1<br />

2 r<br />

0<br />

0<br />

Together with the formula for 1 F⊲rA⊳ this yields the average occurrence of<br />

r amplitudes which exceed a limit rA during a period T:<br />

�<br />

z⊲rA⊳ D Tf0 exp<br />

2<br />

rA �<br />

2 2 r<br />

Often we are interested in questions such as, ‘How is the probability that during<br />

aperiodT a certain stress is exceeded in a structure or an opening is flooded?’<br />

Generally, the issue is then the probability P0⊲rA⊳ that during a period T the<br />

limit rA is never exceeded. In other words, P0⊲rA⊳ is the probability that the<br />

maximum amplitude during the period T is less than rA. Thisisgivenbythe<br />

sum function of the distribution of the maximum or r during T. Wemaketwo<br />

assumptions:<br />

ž z⊲rA⊳ − Tf0; this is sufficiently well fulfilled for rA ½ 2 r.<br />

ž An amplitude rA is statistically nearly independent of its predecessors. This<br />

is true for most seakeeping responses, but not for the weakly damped amplitudes<br />

of elastic ship vibration excited by seaway, for example.<br />

Under these assumption we have:<br />

P0⊲rA⊳ D e z⊲rA⊳<br />

If we insert here the above expression for z⊲rA⊳ we obtain the ‘double’ exponential<br />

distribution typical for the distribution of extreme values:<br />

P0⊲rA⊳ D e Tf0 exp⊲ r 2 A /⊲2 2 r ⊳⊳<br />

The probability of exceedence is then 1 P0⊲rA⊳. Under the (far more limiting)<br />

assumption that z⊲rA⊳ − 1 we obtain the approximation:<br />

1 P0⊲rA⊳ ³ z⊲rA⊳<br />

The equations for P0⊲rA⊳ assume neither a linear correlation of the response r<br />

from the wave amplitude nor a stationary seaway. They can therefore also be<br />

applied to results of non-linear simulations or long-term distributions.<br />

4.4.7 Simulation methods<br />

The appropriate tool to investigate strongly non-linear ship reactions are<br />

simulations in the time domain. The seaway itself is usually linearized,<br />

i.e. computed as superposition of elementary waves. The frequencies of the<br />

individual elementary waves ωj may not be integer multiples of a minimum<br />

frequency ωmin. In this case, the seaway would repeat itself after 2 /ωmin<br />

unlike a real natural seaway. Appropriate methods to chose the ωj are:

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