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Design and Stress Analysis of Extraterrestrial ... - The Black Vault

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Ir<br />

account variation in the modulus <strong>of</strong> elasticity due to nonuniform<br />

heating <strong>of</strong> the blade longitudinally. the values <strong>of</strong> F <strong>and</strong> I<br />

are obtained from gas-dynamic analysis.<br />

"(Z)<br />

Fig. 3.25. Normalizing a function. 2,0 '--<br />

1,6 /<br />

0, - ).8- 0 -- •<br />

0,8 / 0,4 R•w<br />

0 0,2 01 o,6 g8 1,0 o<br />

Fig. 3.26. <strong>The</strong> initial <strong>and</strong><br />

two subsequent approximations t7<br />

<strong>of</strong> the first form <strong>of</strong> the 10--<br />

elastic line <strong>of</strong> a vibrating<br />

blade<br />

calculation).<br />

(example <strong>of</strong> U, -<br />

-<br />

0,6- - -<br />

O24-----------<br />

41<br />

9 7 0<br />

For analysis the blade is<br />

divided into ten equal sections<br />

(generally we can take any number <strong>of</strong> sections <strong>and</strong> they do not have<br />

to be equal).<br />

As the zero approximation we take the elastic line<br />

<strong>of</strong> a cantilever <strong>of</strong>' constant cross section (function<br />

wIO), which<br />

277

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