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

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y<br />

ii<br />

y0<br />

\<br />

1<br />

0-1<br />

H t ieemNw<br />

idn 5ai7<br />

(1)<br />

o NW, (2) U)<br />

'<br />

Fidl'iul<br />

Fig. 3.65. <strong>The</strong> concepts <strong>of</strong> Fig. 3.66. <strong>The</strong> precession<br />

"rigid<br />

<strong>of</strong> a<br />

shaft" <strong>and</strong> "flexible shaft with a disk.<br />

shaft".<br />

KEY: (1) Rigid shaft, (2)<br />

Flexible shaft.<br />

Formula (3.104) for critical. angular velocity is valid only<br />

for the case when a disk is located precisely in the middle between<br />

supports <strong>and</strong> during rotation the shaft is displaced in a parallel<br />

manner without rotation relative to the diameter.<br />

In the overwhelming number <strong>of</strong> cases a disk is locate2 a!,ymmetri-.<br />

cally on the shaft <strong>and</strong>, simultaneously with the revolution around<br />

its own axis with angular velocity w, it rotates along with the<br />

elastlc line relative to the axis <strong>of</strong> the bearings with angular<br />

velocity X. This can be represented as the vibrations <strong>of</strong> a shaft<br />

rotating along with the disk with angular velocity w relative to<br />

axis 01 - 01 in a plane rotating with angular velocity X relative to<br />

axis 0 - 0 (Fig. 3.66). <strong>The</strong> projection <strong>of</strong> the disk onto a thick<br />

plane will complete the oscillating motions (to rotate around its<br />

own diameter).<br />

I<br />

Such qomplex motion <strong>of</strong> bodies in mechanics is called precession<br />

while angular velocity X <strong>of</strong> the elastic line with the disk is called 7<br />

the angular velocity <strong>of</strong> precession or the angular frequency <strong>of</strong><br />

natural (free) vibrations <strong>of</strong> the rotating shaft.<br />

precessive motion are:<br />

Two cases <strong>of</strong><br />

356

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