Considering a multi-body floating system
consisting of N structures, let
the initial estimate of the structure positions and orientations be
represented by the vector ,
(11–9) |
where are the coordinates of
the j-th structure center of gravity
with respect to the FRA, and
are the finite angular
rotations describing the orientation of this structure; the superscripts
denote the iteration step. The displacement required in step 1 is
given by
(11–10) |
and the new position of the body is given by
(11–11) |
The process is repeated until the m-th iterative step, when is
smaller than the prescribed limit for convergence.
It is possible to have more than one
equilibrium position: for example, a capsized ship can still float
in equilibrium, if buoyancy is preserved. It is therefore important
to start the iterative process with an initial estimate that is close
to the required solution. Furthermore, because of the nonlinearities
in the system, it is also possible to overshoot the intended equilibrium
position. In practice,
may therefore be scaled by a specified
under-relaxation factor to ensure stability in the iterative scheme.
Before equilibrium is reached, a set of unbalanced residual forces and moments will act on the bodies. These include hydrostatic forces, weights of the structures, mooring tensions, wind and current drag, thruster forces, steady wave drift forces, and constraint reaction forces as described in External Static Forces and Articulations Between Structures.