15.11.2014 Views

ssc-367 - Ship Structure Committee

ssc-367 - Ship Structure Committee

ssc-367 - Ship Structure Committee

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

X(w) = A*RAO(w)*cos(wt+ O(W)).<br />

When a spectral analysis is applied to the transfer function the<br />

wave amplitudes, A, become a function of wave frequency, u, and<br />

the X(U) is replaced by the differential slice of the response<br />

power density spectrum.<br />

SR(m)*dm = [A(W)*RAO(U)]2<br />

or<br />

SR(w)*dw = A2(u)*RA02(w)<br />

or<br />

SR(~)*dw = S(w)*du*RA02(w)<br />

Thus, Sf(w) = S(U)*RA02(W)<br />

The<br />

the<br />

response spectrum S(W)<br />

RAO squared.<br />

is therefore just the sea spectrum times<br />

For multiple-degree-of-freedom systems, there is coupling between<br />

some of the motions, such as pitch and heave. For example, to obtain<br />

the motion or motion RAO for heave of a point distant from the center<br />

of pitch rotation, the pitch times rotation arm must be added to the<br />

structure heave. This addition must be added with proper<br />

consideration of the relative phase angles of the pitch and heave<br />

motions, and therefore, such addition must be performed at the<br />

regular wave analysis stage. The combined heave (w/pitch) RAO can<br />

then be used in a spectral analysis to obtain the heave spectrum and<br />

heave response characteristicsat the point.<br />

6-7

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!