Practical Ship Hydrodynamics
Practical Ship Hydrodynamics
Practical Ship Hydrodynamics
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Resistance and propulsion 95<br />
resistance tests or propulsion tests with non-cavitating stock propellers<br />
are performed and combined with open-water tests in a cavitation tunnel.<br />
– Surface-piercing propellers<br />
Surface-piercing or ventilated propellers operate directly at the free<br />
surface. Thus the suction side is ventilated and therefore the collapse of<br />
cavitation bubbles on the blade surface is avoided. Due to the operation at<br />
the free surface, Froude similarity has to be maintained in model tests. On<br />
the other hand, thrust and torque, but more important also the side and<br />
vertical forces, strongly depend on the cavitation number. The vertical<br />
force may amount up to 40% of the thrust and therefore will strongly<br />
influence the resistance of planing vessels or SES, ships where this type<br />
of propeller is typically employed.<br />
ž Waterjet propulsion<br />
A common means of propulsion for high-speed ships is the waterjet.<br />
Through an inlet in the bottom of the craft water enters into a bent duct to the<br />
pump, where the pressure level is raised. Finally the water is accelerated and<br />
discharged in a nozzle through the transom. Power measurements on a model<br />
of the complete system cannot be properly correlated to full scale. Only the<br />
inlet and the nozzle are built to scale and an arbitrary model pump with<br />
sufficient capacity is used. The evaluation of waterjet experiments is difficult<br />
and involves usually several special procedures involving a combination of<br />
computations, e.g. the velocity profile on the inlet by boundary layer or<br />
RANSE computations, and measured properties, e.g. pressures in the nozzle.<br />
The properties of the pump are determined either in separate tests of a larger<br />
pump model, taken from experience with other pumps, or supplied by the<br />
pump manufacturer. A special committee of the ITTC was formed to cover<br />
waterjet propulsion and latest recommendation and literature references may<br />
be found in the ITTC proceedings.<br />
3.7 Exercises: resistance and propulsion<br />
Solutions to the exercises will be posted on the internet (www.bh.com/companions/0750648511)<br />
1. A 6 m model of a 180 m long ship is towed in a model basin at a speed of<br />
1.61 m/s. The towing pull is 20 N. The wetted surface of the model is 4 m 2 .<br />
Estimate the corresponding speed for the ship in knots and the effective<br />
power PE using simple scaling laws, i.e. assuming resistance coefficients<br />
to be independent of scale.<br />
2. A ship model with scale D 23 was tested in fresh water with: RT,m D<br />
104.1N, Vm D 2.064 m/s, Sm D 10.671 m 2 , Lm D 7.187 m.<br />
Both model and ship are investigated at a temperature of 15°.<br />
(a) What is the prediction for the total calm-water resistance in sea water<br />
of the full-scale ship following ITTC’57? Assume cA D 0.0002.<br />
(b) What would be the prediction following ITTC’78 with a form factor<br />
k D 0.12? Assume standard surface roughness. Neglect air resistance.<br />
3. A base ship (Index O) has the following main dimension: Lpp,O D 128.0m,<br />
BO D 25.6m,TO D 8.53 m, CB D 0.565 m. At a speed VO D 17 kn, the ship<br />
has a total calm-water resistance of RT,O D 460 kN. The viscosity of water<br />
is D 1.19 Ð 10 6 m 2 /sand D 1025.9 kg/m 3 .