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And<br />

ROTOR THEORY<br />

In the above F refers to a correction factor that takes into account tip losses, according to<br />

Prandtl’s theory. Tip losses occur when air flows around the tip from the lower to upper<br />

surface due to pressure difference.<br />

Cx and Cy are the components of the lift and drag coefficients:<br />

�’ in (B.3) and (B.4) is the solidity ratio, defined as<br />

In case a of (B.3) becomes greater than ac = 0.2 it is no longer valid and the axial interfer-<br />

ence factor is then recalculated by<br />

Where<br />

�<br />

a' =<br />

a =<br />

(B.3)<br />

(B.4)<br />

(B.5)<br />

(B.6)<br />

(B.7)<br />

(B.8)<br />

(B.9)<br />

(B.10)<br />

Combining the above geometric and aerodynamic relations with element theory, it is pos-<br />

sible to calculate the differential axial force and torque acting on a blade element. U<strong>sin</strong>g<br />

this theory, the following assumptions are made:<br />

F<br />

1<br />

4F <strong>sin</strong> ( �)<br />

2<br />

�' C y<br />

1<br />

� 1<br />

4F <strong>sin</strong> ( �)<br />

cos( �)<br />

�' C x<br />

�<br />

� B R�r �<br />

2 � �<br />

2 r <strong>sin</strong>( �)<br />

= acos e<br />

�<br />

�<br />

�<br />

� 1<br />

�<br />

��<br />

��<br />

�<br />

Cx = Cl <strong>sin</strong> ( �)<br />

� Cd cos( �)<br />

Cy = Cl cos( �)<br />

� Cd <strong>sin</strong> ( �)<br />

�'<br />

c B<br />

=<br />

2� r<br />

1<br />

a<br />

2 2 K 1 2a = � � � � c�<br />

� �� K 1 � 2ac K =<br />

� � � 2<br />

4F <strong>sin</strong> ( �)<br />

2<br />

�' C y<br />

� �<br />

�� 2<br />

2<br />

� 4 K ac � 1<br />

�<br />

�<br />

133

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