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5003 Lectures - Faculty of Engineering and Applied Science

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E<strong>5003</strong> - Ship Structures I 52<br />

© C.G. Daley<br />

or much longer than the vessel, the bending moments will be less than if the<br />

wavelength equals the ship length.<br />

Consequently, the design wave for any vessel will have a wavelength equal to the<br />

vessel length. The wave height is also constrained. Waves will have a limited height<br />

to length ratio, or they will break. This results in a st<strong>and</strong>ard design wave <strong>of</strong> L/20. In<br />

other words the wave height (peak to trough) is 1/20 th <strong>of</strong> the wave length.<br />

Trochoidal Wave Pr<strong>of</strong>ile<br />

Note that the waves sketched above did not look like sinusoids. Waves at sea tend<br />

to be trochoidal shaped, rather than simple sine waves. This has the feature that<br />

the crests are steeper <strong>and</strong> the troughs are more rounded.<br />

A trochoidal wave is constructed using a rolling wheel.<br />

In the case <strong>of</strong> the design wave;<br />

LW = LBP<br />

HW = LBP/20<br />

We can see that;<br />

LW = 2 π R<br />

HW = 2 r<br />

}<br />

for now we assume that this length <strong>and</strong><br />

height or wave is possible

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