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Final report for WP4.3: Enhancement of design methods ... - Upwind

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UPWIND WP4: Offshore Support Structures and Foundations<br />

unrestrained motion (surge) [m]<br />

0.05<br />

0.04<br />

0.03<br />

0.02<br />

0.01<br />

0<br />

-0.01<br />

-0.02<br />

Monochromatic wave (T=5 s; H=1 m)<br />

-0.03<br />

0 5 10 15<br />

Time [s]<br />

unrestrained motion (surge) [m]<br />

0.06<br />

0.04<br />

0.02<br />

0<br />

-0.02<br />

-0.04<br />

-0.06<br />

Monochromatic wave (T=7 s; H=2 m)<br />

-0.08<br />

0 5 10 15 20 25<br />

Time [s]<br />

113<br />

unrestrained motion (surge) [m]<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

-0.2<br />

-0.4<br />

-0.6<br />

Monochromatic wave (T=9 s; H=4 m)<br />

-0.8<br />

0 5 10 15<br />

Time [s]<br />

20 25 30<br />

Figure 8.27: Comparison <strong>of</strong> first and second-order unrestrained surge motion <strong>for</strong> the semi-submersible plat<strong>for</strong>m <strong>for</strong> three<br />

monochromatic waves.<br />

unrestrained motion (pitch) [deg]<br />

0.03<br />

0.02<br />

0.01<br />

0<br />

-0.01<br />

Monochromatic wave (T=5 s; H=1 m)<br />

-0.02<br />

0 5 10 15<br />

Time [s]<br />

unrestrained motion (pitch) [deg]<br />

0.1<br />

0.05<br />

0<br />

-0.05<br />

-0.1<br />

Monochromatic wave (T=7 s; H=2 m)<br />

-0.15<br />

0 5 10 15 20 25<br />

Time [s]<br />

unrestrained motion (pitch) [deg]<br />

0.5<br />

0<br />

Monochromatic wave (T=9 s; H=4 m)<br />

-0.5<br />

0 5 10 15<br />

Time [s]<br />

20 25 30<br />

Figure 8.28: Comparison <strong>of</strong> first and second-order unrestrained pitch motion <strong>for</strong> the semi-submersible plat<strong>for</strong>m <strong>for</strong> three<br />

monochromatic waves.<br />

Second-order hydrodynamic loads and unrestrained motions <strong>for</strong> mixed seas<br />

This section presents comparisons between first and second-order excitation <strong>for</strong>ces and unrestrained motions<br />

<strong>for</strong> the semi-submersible plat<strong>for</strong>m, <strong>for</strong> three sea states described by Pierson-Moskowitz distributions with the<br />

parameters listed in Table 8.16. The absolute values <strong>of</strong> the sum- and difference- frequency <strong>for</strong>ce QTFs ( ,<br />

) <strong>for</strong> the semi-submersible plat<strong>for</strong>m in the six modes <strong>of</strong> motion can be found in Appendix B <strong>of</strong> [111].<br />

Pierson-Moskowitz spectrum with Hs=0.5 m<br />

The comparisons between first and second-order excitation <strong>for</strong>ces in the six modes <strong>of</strong> motion (surge, sway,<br />

heave, roll, pitch and yaw) <strong>for</strong> the semi-submersible plat<strong>for</strong>m associated with this spectrum are presented in<br />

Figure 8.29. For this spectrum and <strong>for</strong> all modes, the second-order excitation <strong>for</strong>ces are dominant relative to<br />

the first-order excitation <strong>for</strong>ces.<br />

The comparisons <strong>of</strong> the first and second-order unrestrained motions in the six modes <strong>for</strong> this spectrum are<br />

shown in Figure 8.30. The unrestrained motions are small in all modes. Slow drift motions can be identified in<br />

all modes except heave. For surge, pitch and yaw, the second-order component <strong>of</strong> the unrestrained motions is<br />

<strong>of</strong> the same order <strong>of</strong> importance as the first-order. For the other modes (sway, heave and roll) the second-order<br />

component is dominant over the first-order.

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