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

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"+ '---_• i~l, ... ii. .. .. - - - - - - -<br />

48 0)8- -L<br />

0,7- - - - -07 I i'<br />

Ih 0)5 FIJ<br />

Op "I IZ2.01 0,"<br />

0,2- 0,1<br />

0 - =\,10- N<br />

o,_i L' -- \\<br />

0 1 2 3 1 5 6 7 8 9 o 0-2 0)2 4q 4 , 86 , 186<br />

, •<br />

(a)<br />

.:(b)<br />

Fig. 2.59. Variation in coefficients k, h, y.<br />

Thus, knowing the values <strong>of</strong> y, we obtain the final equation'<br />

for calculating circular perforated plates. <strong>The</strong> initial equations<br />

(2.64) <strong>and</strong> (2.53) for the calculation will-have the folldwing form<br />

W 6pr4,. r 2 C 4 ;<br />

1r .- D1, " r<br />

11 . =9 - Dy -I " .<br />

r (2.81)<br />

When the bending moments <strong>of</strong> an unperforatedd plate are comp uted<br />

<strong>and</strong> it is necessary to determine the stresses in it after perforation,<br />

in the formula <strong>of</strong> stresses (2.56) we should take the thickness <strong>of</strong><br />

the plate, with all3wance for perforation, hn hI, <strong>and</strong> compute2<br />

the stresses from the formulas<br />

rw !<br />

For example, the stresses in a perforated plate, whose seal<br />

has a diagram similar to the one presented in Fig. 2,57, will be:<br />

187

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