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

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-B -<br />

r 2S<br />

dr +ha•,<br />

.1 r(3.87)<br />

Ir<br />

is<br />

a rB<br />

For a disk with a central opening ara is known. Constant B<br />

determined from the known load on the outer loop (when r = RB<br />

Orn). a<br />

For a solid disk, in order not to pass to the limit when r = 0,<br />

we assume that up to a certain small value <strong>of</strong> r = Ra the equality<br />

ara = aqa is preserved (usually, in this case, we assume Ra = O.1Rs).<br />

<strong>The</strong>n from equation (3.86) we obtain<br />

'B=Ra, a•a- (3.88)<br />

is<br />

In equation (3.86) there remains one unknown quantity ara, which<br />

determined from the known load on the outer loop.<br />

Usually no less than two approximations are made for ar in order<br />

to assure the accuracy <strong>of</strong> the obtained results, especially as the<br />

determination <strong>of</strong> ar2 does not require a large amount <strong>of</strong> computation.<br />

Without making the first approximation <strong>of</strong> (Pl, we immediately<br />

determine ar2' From equality (3.84) we find the difference<br />

(a•I - arl) after the substitution into this equality <strong>of</strong> the value<br />

<strong>of</strong> arl:<br />

0] +,)EI<br />

%i -- ,i = rl+,• r~aidr -- cit -- 1 - ) , -<br />

P Ra<br />

•(l-Pl)-I r•'"dr-m-A<br />

. r " (3.89)<br />

337

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