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The following assumptions are made when u<strong>sin</strong>g the above calculation principle:<br />

� The rotor plane is perpendicular to the direction of the wind<br />

� Friction in the tail pivot is neglected<br />

� The mass of welds in the tail is neglected<br />

� The tail vane is parallel to the air flow<br />

FURLING AND YAW ANALYSIS<br />

The gain height Δh of the tail is analysed in SolidWorks as a function of the furling angle �f<br />

in the range of 0-5�, u<strong>sin</strong>g 1� steps.<br />

Furling angle, �f [�] Height gained, Δh [mm]<br />

Table I.2: Results of the tail motion analysis<br />

0 0<br />

1 9.28<br />

2 18.8<br />

3 28.4<br />

4 38.3<br />

5 48.3<br />

The rotor thrust Ftf is calculated for wind speeds 13 m/s, 14 m/s and 15 m/s as shown in<br />

table I.3.<br />

Wind speed V [m/s] 13 14 15<br />

Thrust force Ftf [N] 718 872 1050<br />

Table I.3: Rotor thrust force as different wind speeds<br />

The work performed by during furling Wr may now be calculated as a function of the furl-<br />

ing angle �f at the three wind speeds of table I.3. Correspondingly the potential energy of<br />

the tail may be calculated as a function of the furling angle �f. The result is illustrated on<br />

figure I.5 below.<br />

209

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