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Digby Symons - Blade

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5.3 Self Weight loading<br />

The bending moment at the blade root due to self weight loading can<br />

dominate the stresses at the blade root. Because the turbine is<br />

rotating the bending moment is a cyclic load with a frequency of<br />

f = ω / 2π<br />

. The maximum self-weight bending moment occurs when a<br />

blade is horizontal.<br />

Fig. 26<br />

Bending moment at root of blade due to self weight<br />

M<br />

sw<br />

=<br />

R<br />

∫<br />

rmin<br />

m(<br />

r)<br />

g(<br />

r − rmin<br />

) dr<br />

where m(r) is the mass of the blade per unit length. This is a<br />

tangential (edge-wise) bending moment and therefore the maximum<br />

bending stress due to self-weight is given by:<br />

σ<br />

M sw b<br />

max, sw =<br />

I NN 2<br />

Simplified method: split blade into elements, assume each element<br />

has uniform self weight.<br />

24

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