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

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<strong>The</strong> selection <strong>of</strong> any form <strong>of</strong> approximating dependence depends<br />

on what kind <strong>of</strong> problem is being solved. For example, in solving<br />

the problem <strong>of</strong> small vibrations in<br />

an unloaded rotor we can limit<br />

ourselves to a linear dependence if the form ( 3 .1 5 4). If, however,<br />

we are examining the effect <strong>of</strong> forced vibrations on modes <strong>of</strong> autovibration<br />

<strong>of</strong> currents or we are examining vibrations whose amplitudes<br />

are commensurate with the value <strong>of</strong> the radial gap in the bearings,<br />

we must take into account the nonlinearity <strong>of</strong> the characteristics<br />

FrO ()<br />

Dependences F to <strong>and</strong> Fc can be approximated by the linear<br />

relationships:<br />

PtAO=aU 2 eVo; FcaWVo. (3.155)<br />

A transition from dimensionless quantities F, c, V0 <strong>and</strong> v0<br />

to dimensioned quanti'ies F, r, w, 6 is effected with the aid <strong>of</strong><br />

the following relationships:<br />

F.=F.pDL,; r=E. 0 to); w= D Q~;=~V<br />

By themselves the dimensioned forces can be written in linear<br />

form: F 1 = kIr; F 2 = k 2 wr; F3 = k 3 v, where subscripts 1, 2, 3<br />

correspond to the former subscripts r, t, c, respectively.<br />

Coefficients kl, k 2 , k 3 are connected with coefficients a,, c 2 ,<br />

ca 3 by relationships:<br />

) L L r 1)L<br />

L o A ,;2=C2 2; 3==3<br />

S I 397

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