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

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

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Substituting the difference (awl - a)rl into equation (3.82), we<br />

obtain the second approximation for ar:<br />

a L1 +1)d rcatdr-Eal hQtl Qw2 rhidr<br />

h r dr ' "E<br />

r-) rs dr-- (I -- #)z, -, L r<br />

r--LazrA 'E<br />

Sfr~I~ * E r r 2 +IL<br />

L Ra (3.90)<br />

<strong>The</strong> constant A for a disk with an opening is determined from the<br />

equation (3.90) with a known load on the outer loop. For a disk<br />

with a central opening when r = R a = a <strong>and</strong> according to<br />

formuLa (3.85)<br />

A ==--• IA1--PY):,a+4-Eaaota].(3)<br />

(3.91)<br />

Substituting this value <strong>of</strong> A into equation (3.90), we determine<br />

ara <strong>and</strong> then all the other values <strong>of</strong> ar2' After determining ar2<br />

(<strong>and</strong> if this approximation is sufficient) we find the values <strong>of</strong><br />

a92 from equation (3.89):<br />

,;2 -- (& - E,.- r•u dr -- E- a -- I " .) -<br />

R a ,<br />

I rl E r+ " (3.92)<br />

Ra<br />

For a solid disk the determination <strong>of</strong> aP2 should begin with<br />

r = R <strong>and</strong> instead <strong>of</strong> the constant A, we. should substitute its value from<br />

formula (3.91).<br />

338

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