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Chapter 3 - Dynamics of Marine Vessels

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40<br />

3.5.3 Longitudinal and Lateral Models<br />

Longitudinal Subsystem (DOFs 1, 3, 5)<br />

For simplicity, it is assumed that higher order damping can be neglected, that is<br />

Dn 0. Coriolis is, however, modelled by assuming that u 0 and that<br />

2nd-order terms in v,w,p,q, and r are small. Hence, DOFs 1, 3, 5 gives:<br />

CRB <br />

CRB ≈<br />

my g q z g rp − mx g q − wq − mx g r vr<br />

−mz g p − vp − mz g q uq mx g p y g qr<br />

mx g q − wu − mz g r xgpv mz g q uw I yz q I xz p − I z rp −I xz r − Ixyq I x pr<br />

Collecting terms in u,w, and q, gives:<br />

0 0 0<br />

0 0 −mu<br />

0 0 mxgu<br />

Assuming a diagonal M A gives:<br />

CA <br />

−Zẇ wq Y v̇ vr<br />

−Y v̇ vp X u̇ uq<br />

u<br />

w<br />

Z ẇ −Xu̇ uw N ṙ −Kṗ pr<br />

q<br />

≈<br />

0 0 0<br />

0 0 Xu̇ u<br />

0 Z ẇ −Xu̇ u 0<br />

CRB ≠−CRB<br />

The skew-symmetric property is<br />

destroyed for the decoupled model:<br />

<br />

u<br />

w<br />

q<br />

Ivar Ihle – TTK4190 Spring 2006

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