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

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<strong>Analysis</strong> <strong>of</strong> critical shaft speed<br />

With the use <strong>of</strong> turbines <strong>of</strong> rapidly revolving shafts a<br />

phenomenonf called "critical rpm" was detected.<br />

It was noticed that during the slow rotation <strong>of</strong> a rotor no<br />

noticeable vibrations are observed. <strong>The</strong> rotor rotates smoothly.<br />

With the achievement <strong>of</strong> a certain number <strong>of</strong> revolutions the rotor<br />

begins, without visible cause, to vibrate sharply, which can lead<br />

to the breakdown <strong>of</strong> a clearly strong shaft.<br />

in revolutions the rotor again begins to rotate quietly.<br />

With a further increase<br />

<strong>The</strong> rpm at whic" a shaft loses stability <strong>and</strong> begins to vibrate<br />

is called critical.<br />

<strong>Stress</strong> analysis <strong>of</strong> shafts is studied in courses on the strength<br />

<strong>of</strong> materials <strong>and</strong> machine parts. <strong>The</strong>refore, in this section we shall<br />

examine only the questions <strong>of</strong> transient stability <strong>of</strong> shafts.<br />

Let us consider a shaft arranged vertically (for the elimination<br />

<strong>of</strong> the effect <strong>of</strong> its weight) in the middle cross section <strong>of</strong> which<br />

is attached a disk with mass m.<br />

Let us assume that the mass <strong>of</strong> the<br />

shaft is low as compared with the mass <strong>of</strong> the disk; however, the<br />

shaft possesses elastic properties. Let us also assume that the<br />

center <strong>of</strong> gravity <strong>of</strong> the disk c is displaced relative to the<br />

geometric center 01 by quantity e (Fig. 3.62). We further assume that<br />

supports allowing the shaft to rotate freely are absolutely rigid.<br />

When the rotor only begins to rotate <strong>and</strong> the elastic axis <strong>of</strong><br />

the shaft is still a straight line (Fig. 3.62a), then, as a result<br />

<strong>of</strong> the displacement <strong>of</strong> the disk's c¢nter <strong>of</strong> gravity with respect<br />

to the axis <strong>of</strong> rotation, there appears centrifugal force mew 2 .<br />

Under the effect <strong>of</strong> this force the shaft begins to be deflected,<br />

which, in turn, leads to an increase in the centrifugal force<br />

2<br />

(Fig. 3.62b): PC m(y + eOw<br />

351

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