Practical Ship Hydrodynamics
Practical Ship Hydrodynamics
Practical Ship Hydrodynamics
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<strong>Ship</strong> manoeuvring 169<br />
the difference between symmetrical and asymmetrical flow is linearized.<br />
The asymmetrical flow is then determined by a lifting body method with an<br />
additional source distribution above the free surface.<br />
ž Field methods<br />
In spite of the importance of viscosity for manoeuvring, viscous hull force<br />
calculations appeared in the 1990s only as research applications and were<br />
mostly limited to steady flow computations around a ship with a constant<br />
yaw angle. Difficulties in RANSE computations for manoeuvring are:<br />
– The number of computational cells is much higher than for resistance<br />
computations, because both port and starboard sides must be discretized<br />
and because vortices are shed over nearly the full ship length.<br />
– The large-scale flow separation makes wall functions (e.g. in the standard<br />
k-ε turbulence model) dubious. But avoiding wall functions increases the<br />
necessary cell numbers further and deteriorates the convergence of the<br />
numerical solution methods.<br />
State of the art computations for ship hulls at model scale Reynolds numbers<br />
were capable of predicting transverse forces and moments reasonably well<br />
for steady flow cases with moderately constant yaw angle, but predicted<br />
the longitudinal force (resistance) with large relative errors. Flow details<br />
such as the wake in the aftbody were usually captured only qualitatively.<br />
Either insufficient grid resolutions or turbulence models were blamed for the<br />
differences with model tests. By the late 1990s, RANSE results with freesurface<br />
deformation (waves) were also presented, but with the exception<br />
of Japanese research groups, none of the computations included dynamic<br />
trim and sinkage, although for shallow water these play an important role<br />
in manoeuvring.<br />
Despite these shortcomings, RANSE computations including free-surface<br />
effects will grow in importance and eventually also drift into practical<br />
applications. They are expected to substantially improve the accuracy of<br />
manoeuvring force predictions over the next decade.<br />
5.3 Experimental approaches<br />
5.3.1 Manoeuvring tests for full-scale ships in sea trials<br />
The main manoeuvring characteristics as listed in the introduction to manoeuvring<br />
are quantified in sea trials with the full-scale ship. Usually the design<br />
speed is chosen as initial speed in the manoeuvre. Trial conditions should<br />
feature deep water (water depth > 2.5 ship draft), little wind (less than Beaufort<br />
4) and ‘calm’ water to ensure comparability to other ships. Trim influences<br />
the initial turning ability and yaw stability more than draft. For comparison<br />
with other ships, the results are made non-dimensional with ship length and<br />
ship length travel time (L/V).<br />
The main manoeuvres used in sea trials follow recommendations of the<br />
Manoeuvring Trial Code of ITTC (1975) and the IMO circular MSC 389<br />
(1985). IMO also specifies the display of some of the results in bridge posters<br />
and a manoeuvring booklet on board ships in the IMO resolution A.601(15)<br />
(1987) (Provision and display of manoeuvring information on board ships).<br />
These can also be found in Brix (1993).