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Practical Ship Hydrodynamics

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

C p = P dyn /q<br />

1.0<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

−0.2<br />

−0.4<br />

−0.6<br />

−0.8<br />

−1.0<br />

−1.2<br />

−1.4<br />

−1.6<br />

−1.8<br />

1.25<br />

1.0<br />

0.75<br />

0.5<br />

0.25<br />

0<br />

0.75<br />

0.25<br />

0.5<br />

1.0<br />

1.25<br />

C Ll as parameter<br />

0.5 1.0<br />

−2.5<br />

−3.0<br />

−3.5<br />

0.1<br />

0.75<br />

1.0<br />

1.25<br />

X / C<br />

Figure 5.17 Distribution of the non-dimensional dynamic pressure along a NACA0021 profile<br />

as a function of the local lift coefficient CLl (Riegels (1958))<br />

sides, respectively. For profiles with a curved mean line, an additional velocity<br />

component has to be added. It may be taken from Abbott and Doenhoff (1959),<br />

pp. 77ff and App. II, or it may be determined by a two-dimensional potentialflow<br />

calculation for which various methods and codes are available. Brix<br />

(1993), p. 84, gives a sample calculation for the NACA643-018 profile for<br />

˛ D 15°.<br />

5.4.3 Rudder types<br />

Various rudder types have been developed over the years (Fig. 5.18):<br />

Simplex rudder Spade rudder Semi-balanced<br />

rudder<br />

Figure 5.18 Various rudder types<br />

Flap rudder

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