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

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Near the faces <strong>of</strong> a shell there will occur a certain bend<br />

as a result <strong>of</strong> the effect <strong>of</strong> its<br />

attachment.<br />

f A4<br />

support.<br />

Let us examine the stresses in a shell if its ends have no<br />

In this case, stresses a, on the end will be equal to zero.<br />

Since the stresses (5.<br />

3 4) can be obtained as a result <strong>of</strong> applying<br />

bending moment to the face <strong>of</strong> the shell, we shall apply moment<br />

0 M= , which is attained by a rigid attachment <strong>of</strong> the shell eril.<br />

With allowance for the sign,<br />

o= S 0 --ax#2EuAth2<br />

X; A1o,= -<br />

12(1 (5.35)<br />

In order to create the same conditions as exist without<br />

attachment <strong>of</strong> the face (ax = 0), Jt is necessary to apply ctistribated<br />

moment <strong>of</strong> the same magnitude but <strong>of</strong> the opposite uign.<br />

in<br />

<strong>Stress</strong>es<br />

a free end will be defined as the sum <strong>of</strong> stresses determined bý<br />

formula (5.34) <strong>and</strong> stresses caused by moment M 0 (Fig. 5.25).<br />

II<br />

ai) (a) 6) (b) o (c)<br />

Fig. 5.25. Determining stresses in the presence <strong>of</strong> a<br />

temperature gradient through the thickness.<br />

are known:<br />

Loads in a free shell causecd by moment M 0 applied tc the end<br />

JPra.ýt2:- 6,1 ;<br />

12(1-p.)' -<br />

AL~o(O) =v,' 0o= Ea~th2.u." " •÷(Al).z •.,. ('l);<br />

a<br />

12(1--p.)<br />

T, (0) Lh [E (0)]=L M •_o 0<br />

r r 2- 2 D<br />

- h 1- . - "(5.36)-<br />

i( .35

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