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YAW AND FURLING<br />

As shown on figure 8.7 the furling axis is tilted compared to the yaw axis. This inclination<br />

causes the tail vane to rise during the furling action, thus creating an increase in the po-<br />

tential energy of the tail vane.<br />

Figure 8.7: Rai<strong>sin</strong>g tail vane. Top: Normal operation. Bottom: Furled operation with inclined<br />

tail vane.<br />

The instantaneous position of the furled rotor is a balance between the gravity force on<br />

the tail vane and the thrust force on the rotor. Equilibrium of the system is established<br />

under stationary conditions when the torque around the yaw axis balances the gravity<br />

torque around the furling axis. When the wind speed decreases below the critical value of<br />

14 m/s, the rotor is automatically recovered from the furled position and realigned with<br />

the wind direction by the restoring moment provided by gravity.<br />

Appendix I.2 verifies the overall functionality of the furling mechanism by confirming<br />

that furling is initiated at a wind speed of 14 m/s (equivalent to a thrust force of 872 N).<br />

The power production beyond the onset of furling is not analysed in the present project,<br />

as it is beyond the limitations of the BEM theory described in appendix B.1.<br />

81

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