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ssc-367 - Ship Structure Committee

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\Lf-!<br />

of cycles. Thus, the reduced velocity necessary for the onset of<br />

cross-flow vibrations in steady current should be avoided.<br />

0.3.3 Critical Flow Velocities<br />

The criteria for determining the critical flow velocities for the<br />

onset of VW can be expressed in terms of the reduced velocity<br />

(Section D.2):<br />

v cr = (Vr)cr (fn* d)<br />

where:<br />

(Vr) Cr = 1.2 for in-line oscillations in water<br />

= 1.7 for in-line oscillations in air<br />

= 3.9 for cross-flow oscillations in water<br />

=<br />

4.7 for cross-flow oscillations in air<br />

0.4. AMPLITUDES OF VIBRATION<br />

Amplitudes of vibrations can be determined by several methods. A DnV<br />

proposed procedure (Reference 0.8) is simple to apply and allows<br />

determination of member natural frequencies, critical velocities and<br />

maximum amplitudes of vortex-shedding induced oscillations. The<br />

procedure yields consistent results, comparable to the results<br />

obtained by other methods, except for oscillation amplitudes. The<br />

DnV calculation of oscillation amplitudes is based on a dynamic load<br />

factor of a resonant, damped, single-degree-of-freedomsystem. this<br />

approach is not valid unless the nonlinear relationship between the<br />

response and damping ratio is known and accounted for. Consequently,<br />

in-line and cross-flow vortex shedding amplitudes are assessed<br />

separately.<br />

D-9

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