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

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Differentiating this equation, we find the expression for<br />

shearing force:<br />

d2M =<br />

dZ'<br />

(c)<br />

After we differentiate equation (c)<br />

for linear load from the internal elastic forces:<br />

once more, we obtain an expression<br />

d2M" __.-L = q =(EI~')".<br />

dz2<br />

dz<br />

(d)<br />

Let us make the external linear load equal to the linear load<br />

from -internal -forces--[equations, (a' -) -<strong>and</strong> (d-)]; -then the general<br />

differential equation for an oscillating blade will be written in<br />

the form<br />

(Ehi')" +eFI--=0. (3.-19),<br />

To solve differential equation -(3.19) ].t us use Fourier t s<br />

method - the separation <strong>of</strong> variables z <strong>and</strong> t. We shall introduce<br />

designations:<br />

Trjz, t)=u(z), g(W)=ug,<br />

where u(z) is the function <strong>of</strong> deflection, depending only on the z<br />

coordinate;<br />

g(t) is the function <strong>of</strong> deflection depending only or time t.<br />

If we differentiate equation (e) four times with respect to<br />

z <strong>and</strong> two times with respect to t <strong>and</strong> substitute these derivatives<br />

into equation (3.19), we obtain<br />

,,,, ' -- , •<br />

(3.20)<br />

262<br />

j

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