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

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Function B(T) is found after determining function ' by graphic<br />

<strong>and</strong> numerical differentiation.<br />

As seen from the figure, the value <strong>of</strong> coefficient. B() is<br />

Svariable in a certain segment -it corresponds to the segment <strong>of</strong><br />

Unsteady cree-i <strong>and</strong> is constant in the remaining segment - the segment<br />

<strong>of</strong> steady creep. Function Q after a certain value grows<br />

monotonically.. •Function p decreases shai'ply when J -near zero<br />

<strong>and</strong> then, monotoni*aliy.<br />

<strong>The</strong>rnrl' stresses<br />

In studying thermal stresses we face two different problems.<br />

<strong>The</strong> first problem is finding the thermal stresses -which appear<br />

as a result <strong>of</strong> rapid heating or cooling <strong>of</strong> a junction or part. This<br />

mode, although brief, corresponds to the -maximum temperature gradients<br />

<strong>and</strong>, consequently, stresses. Decrease in these stresses can be<br />

achieved by increasing unit firing time or starting time. For an<br />

installation where the time must be minimal, stresses must be<br />

designed for.<br />

<strong>The</strong> second problem is<br />

to calculate stresses which occur in<br />

parts. as a- result <strong>of</strong> the effect <strong>of</strong> steady thermal fluxes <strong>and</strong><br />

their corresponding steady temperature gradients.<br />

For very many elements this calculat16n.-is fundamental if<br />

deformations corresponding ho these stresses do not go beyond the limits<br />

<strong>of</strong> elastic. This calculation can be a reference for stress analysis<br />

if thermal stre.-ses exceed the elasticity limit <strong>of</strong> the material<br />

when plastic deformations accompanying these sti-esses dan not be<br />

disregarded. Strength calculation for parts) in this ca~'e, must<br />

be made with relaxation phenomena taken into account.<br />

81

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