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ssc-367 - Ship Structure Committee

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their function, selecting appropriate element aspect ratios (less<br />

than 1:2) will contribute both to better accuracy and a better<br />

model.<br />

5.2.2<br />

Stationary Marine <strong>Structure</strong>s<br />

Determination of Loads<br />

Stationarymarine structureshavevariousconfigurationsand exhibit<br />

a wide range of compliancy. A substantial effort is desirable to<br />

minimize the fatigue loadings on stationary structures. For a<br />

moored tanker FPSO the smallestfunctionalsize exhibitinga minimum<br />

silhouette is desirable. For structures composed of columns and<br />

pontoons, the column spacing,column water plane area, displacement<br />

of pontoons affecting overall center of buoyancy and the total<br />

displacement are some of the interactingparameters that affect not<br />

only the magnitude and characterof the applied loading but also the<br />

response of the structureto applied loading (see Reference 5.6 for<br />

structure configurationoptimization).<br />

While the hydrodynamic forces on a slender stationary body can be<br />

determined based on strip method or diffraction theory, a structure<br />

made up of columns and pontoons can be determined either by<br />

Morison’s equation or by diffraction theory. As discussed in<br />

Section 5.1, large diameters disturb the flow, leading to<br />

diffraction which is highly frequency dependent. There are two<br />

benefits of using diffraction theory:<br />

●<br />

Diffraction usually causes a reduction in the wave loads,<br />

●<br />

Viscosity can be ignored and thus, treating the flow as<br />

irrotational,potential flow theory may be used.<br />

The hydrodynamicloads actingon astructure are typically generated<br />

using a combination of three-dimensionaldiffraction theory, i.e.,<br />

a source-sink distributed potential theory (Reference 5.7) and a<br />

conventional Morison’s equation. Although a two-dimensional<br />

5-1o<br />

/ 1A

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