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Friction forces and moments<br />

FURLING AND YAW ANALYSIS<br />

(I.13)<br />

The friction force in the bearings is calculated from the sum of the reaction force in the two<br />

bearings, which is:<br />

U<strong>sin</strong>g a friction coefficient µs of 0.2, the friction force becomes:<br />

This is recalculated into a frictional resistance moment:<br />

A total frictional resistance moment is calculated by further adding the required starting<br />

(I.14)<br />

(I.15)<br />

(I.16)<br />

torque for the thrust bearing Mst, which is 28.8 Nmm. The calculation, which is documented<br />

in att. 3, uses the following input:<br />

� Bearing load: 997 N<br />

� The number of rotations per minute: 1 rpm<br />

� Friction coefficient in full-film condition: 0.1 µEHL, which corresponds to grease<br />

used as lubrication in the bearing.<br />

Yawing moment<br />

The aerodynamic lift and drag forces on the tail vane will tend to align the rotor with the<br />

wind, whereas the thrust force on the rotor and the above calculated frictional resistance<br />

(I.17)<br />

moment will oppose the tendency. U<strong>sin</strong>g principles of equilibrium it is possible to calculate<br />

a steady state yaw offset.<br />

The lift force is perpendicular to the wind direction and the drag is parallel to the wind<br />

direction, which is shown on the free body diagram of the tail vane and the rotor on figure<br />

I.3.<br />

RB Rx.B 2 Ry.B 2<br />

� � � 354 N<br />

Rtot � RA � RB � 721N<br />

Ffr � Rtot s � 144N<br />

Mfr �<br />

Db<br />

Ffr<br />

2<br />

� 6.70Nm<br />

Mfr.tot �<br />

Mst � Mfr � 6.73Nm<br />

205

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