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ssc-367 - Ship Structure Committee

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a<br />

fn = ~ (EI/mi L4)%<br />

where:<br />

the<br />

moment of inertia of the beam<br />

3.52 for a beam with fix-free ends (cantilever)<br />

9.87 for a beam with pin-pin ends<br />

15.4 for a beam with fix-pin ends<br />

22.4 for a beam with fix-fix ends<br />

1ength<br />

mode of vibration<br />

mass per unit length<br />

The amount of member fixity assumed in the analysis has a large<br />

effect on vortex shedding results, because of its impact on member<br />

stiffness, natural period, amplitude of displacement, and member<br />

stress. Hence, careful consideration should be given to member end<br />

conditions. Members framing into relatively stiff members can<br />

usually be assumed to be fixed. Other members, such as caissons and<br />

risers, may act as pinned members if supports are detailed to allow<br />

member rotation.<br />

For members with non-uniform spans, complex support arrangements or<br />

non-uniform mass distribution, the natural frequency should be<br />

determined from either a dynamic analysis or from Tables provided in<br />

References D.5 and D.6. Reid (Reference D.7) provides a discussion<br />

and a model to predict the response of variable geometry cylinders<br />

subjected to a varying flow velocities.<br />

The natural frequency of a member is a function of the member’s<br />

stiffness and mass. For the purposes of vortex shedding analysis and<br />

design, the member’s stiffness properties are computed from the<br />

D-6

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