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LIST OF ATTACHMENTSBASIS FOR CALCULATIONS<br />
Load case B: Yawing<br />
For this load case the ultimate loads during yawing are calculated for the blades and shaft.<br />
The flapwise bending moment acting on the blades is considered to consist of three terms:<br />
126<br />
� Centrifugal force<br />
� Gyroscopic<br />
� Eccentricity of axial load<br />
The first two terms occur due to the maximum yaw speed �yaw which is considered to oc-<br />
cur with �design.<br />
The last term accounts for an offset of the axial force, similar to that of (A.8).<br />
For each blade the formula for the flapwise bending moment is:<br />
(A.9)<br />
(A.10)<br />
The centrifugal force due to the yaw rate is multiplied by the distance Lrt of figure A.2. The<br />
gyroscopic term is elaborated further in [5, p. 165].<br />
For the shaft the bending moment is given by:<br />
(A.11)<br />
The load consists of a gyroscopic load valid for a three bladed rotor and two terms adding<br />
mass loads and axial load eccentricity.<br />
Load case C: Yaw error<br />
� �<br />
�yaw 3 0.01 � R 2<br />
= � � 2 2.96 rad<br />
=<br />
s<br />
2 R<br />
MyB mB �yaw Lrt Rcog � 2�yaw IB �design 9 �F �<br />
� xS � 98.6 N m<br />
R<br />
MS B�yaw �design IB � mr g Lrb 6 �F �<br />
� xS � 179 N m<br />
All turbines operate with a certain yaw error. In this load case, a yaw error of 30° is con-<br />
sidered to induce a blade root bending moment. It is derived u<strong>sin</strong>g approximations that<br />
simplify a condition, where an extreme load is caused by the combination of the instanta-<br />
neous wind and the yaw error, which is thought to place the entire blade at the angle of<br />
attack for maximum lift. Further details may be found in [5, p. 169].<br />
1<br />
MyB 8 � Aproj.B Cl.maxR 3 � 2 4<br />
�<br />
�design �1<br />
� �<br />
� 3�design �<br />
�<br />
�<br />
1<br />
� design<br />
2<br />
� �<br />
� �<br />
� �<br />
� 200 N m<br />
(A.12)