Practical Ship Hydrodynamics
Practical Ship Hydrodynamics
Practical Ship Hydrodynamics
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<strong>Ship</strong> manoeuvring 171<br />
it is important to consider that the ship is faster at the beginning of the<br />
turning circle and slower at sustained turning. The heeling angle exceeds<br />
dynamically the statical heel angle due to forces listed above.<br />
The turning circle test is used to evaluate the turning ability of the ship.<br />
2. Spiral manoeuvres<br />
We distinguish between:<br />
– ‘Direct’ spiral manoeuvre (Dieudonne)<br />
With the ship on an initial straight course, the rudder is put hard to one<br />
side until the ship has reached a constant rate of change of heading.<br />
The rudder angle is then decreased in steps (typically 5°, but preferably<br />
less near zero rudder angle) and again held until a steady condition is<br />
reached. This process is repeated until the rudder has covered the whole<br />
range to the maximum rudder angle on the other side. The rate of turn<br />
is noted for each rudder angle. The test should be performed at least for<br />
yaw unstable ships going both from port to starboard and from starboard<br />
to port.<br />
– ‘Indirect’ (reverse) spiral manoeuvre (Bech)<br />
The ship is steered at a constant rate of turn and the mean rudder angle<br />
required to produce this yaw rate is measured. This way, points on the<br />
curve rate of turn vs. rudder angle may be taken in any order.<br />
The spiral test results in a curve as shown in Fig. 5.5. The spiral test is used<br />
to evaluate the turning ability and the yaw stability of the ship. For yaw<br />
unstable ships, there may be three possible rates of turn for one given rudder<br />
angle as shown in Fig. 5.5. The one in the middle (dotted line) represents<br />
an instable state which can only be found by the indirect method. In the<br />
direct method, the rate of turn ‘switches’ at the vertical sections of the<br />
curve suddenly to the other part of the curve if the rudder angle is changed.<br />
This is indicated by the dotted arrows in Fig. 5.5.<br />
Rate of turn Rate of turn<br />
Right (stb)<br />
Curve obtained<br />
from reversed<br />
spiral<br />
Rudder angle d<br />
Rudder angle d<br />
Left (port) Right (stb) Left (port)<br />
Right (stb)<br />
Left (port)<br />
Figure 5.5 Results of spiral tests for yaw stable and yaw unstable ship<br />
Right<br />
Left<br />
(stb)<br />
(port)<br />
Curve obtained<br />
from direct or<br />
reversed spiral<br />
The spiral test, especially with the direct method, is time consuming and<br />
sensitive to external influences. The results show that a linearization of the<br />
body force equations is acceptable only for small jrj (Fig. 5.5). For yaw<br />
stable ships, the bandwidth of acceptable rudder angles to give small jrj is<br />
small, e.g. š5°. For yaw unstable ships, large jrj may result for any υ.