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Practical Ship Hydrodynamics

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76 <strong>Practical</strong> <strong>Ship</strong> <strong>Hydrodynamics</strong><br />

is in self-propelled equilibrium. Usually the speed of the towing tank carriage<br />

is kept constant and the rpm of the propeller varied until an equilibrium is<br />

reached. A propeller dynamometer then measures thrust and torque of the<br />

propeller as a function of speed. In addition, dynamical trim and sinkage<br />

of the model are recorded. The measured values can be transformed from<br />

model scale to full scale by the similarity laws: speed Vs D p Ð Vm, rpm<br />

ns D nm/ p 3 4 , thrust Ts D Tm Ð ⊲ s/ m⊳ Ð , torque Qs D Qm Ð ⊲ s/ m⊳ Ð .A<br />

problem is that the propeller inflow is not geometrically similar for model and<br />

full scale due to the different Reynolds number. Thus the wake fraction is also<br />

different. Also, the propeller rpm should be corrected to be appropriate for the<br />

higher Reynolds number of the full-scale ship.<br />

The scale effects on the wake fraction are attempted to be compensated by<br />

the empirical formula:<br />

ws D wm Ð cFs<br />

� �<br />

cFs<br />

C ⊲t C 0.04⊳ Ð 1<br />

cFm<br />

cFm<br />

t is the thrust deduction coefficient. t is assumed to be the same for model and<br />

full scale.<br />

The evaluation of the propulsion test requires the resistance characteristics<br />

and the open-water characteristics of the stock propeller. There are two<br />

approaches:<br />

1. ‘Thrust identity’ approach<br />

The propeller produces the same thrust in a wake field of wake fraction w<br />

as in open-water with speed Vs⊲1 w⊳ for the same rpm, fluid properties<br />

etc.<br />

2. ‘Torque identity’ approach<br />

The propeller produces the same torque in a wake field of wake fraction w as<br />

in open-water with speed Vs⊲1 w⊳ for the same rpm, fluid properties etc.<br />

ITTC standard is the ‘thrust identity’ approach. It will be covered in more<br />

detail in the next chapter on the ITTC 1978 performance prediction method.<br />

The results of propulsion tests are usually given in diagrams as shown<br />

in Fig. 3.9. Delivered power and propeller rpm are plotted over speed. The<br />

results of the propulsion test prediction are validated in the sea trial of the<br />

ship introducing necessary corrections for wind, seaway, and shallow water.<br />

The diagrams contain not only the full-load design condition at trial speed, but<br />

also ballast conditions and service speed conditions. Service conditions feature<br />

higher resistance reflecting the reality of the ship after some years of service:<br />

increased hull roughness due to fouling and corrosion, added resistance in<br />

seaway and wind.<br />

3.2.8 ITTC 1978 performance prediction method<br />

The ITTC 1978 performance prediction method (IPPM78) has become a<br />

widely accepted procedure to evaluate model tests. It combines various aspects<br />

of resistance, propulsion, and open-water tests. These are comprehensively<br />

reviewed here. Further details may be found in section 3.2.5, section 3.2.7<br />

and section 2.5, Chapter 2. The IPPM78 assumes that the following tests have

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