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

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! t<br />

I<br />

<strong>The</strong> frequency characteristic is<br />

symmetric relative to the<br />

origin <strong>of</strong> coordinates.<br />

This means that the curvesicoincide exactly'<br />

in the ! <strong>and</strong> III <strong>and</strong> in the II <strong>and</strong> IV quadrants. <strong>The</strong>refore, they<br />

are bounded by its representation only in the two neighboring<br />

quadrants: in I <strong>and</strong> II (Fig. 3.73a') or in I <strong>and</strong> IV (Fig. 3.73b).<br />

<strong>The</strong> latter representation more accurately eýresses the physical<br />

essence: for a given direction <strong>of</strong> shaft rotation'(we assume it is<br />

positive) both forward (positive values <strong>of</strong> X),<br />

(negative values <strong>of</strong> X) occur.<br />

anrd reversp precession<br />

However, from the mathematical point<br />

<strong>of</strong> view, it is more convenient to deal with continuous curves, i.e.,<br />

with the representation <strong>of</strong> characteristics as shown in<br />

Fig. 3.73a.<br />

<strong>Analysis</strong> <strong>of</strong> the frequency characteristic shows that in the<br />

examined single-disk system each value <strong>of</strong> angular velocity<br />

corresponds to two natural angular frequencies (velocities') in the!<br />

region <strong>of</strong> forward precession <strong>and</strong> two in the region <strong>of</strong>reverse<br />

precession. For the entir, set <strong>of</strong> angular shaft velocities-there -<br />

is an infinite number <strong>of</strong> natural angular frequencies.<br />

Fig. 3.74. Shapes <strong>of</strong> the elastic<br />

line during the vibration <strong>of</strong> a<br />

rotating shaft with one disk.<br />

a~ .(a) 6)(b) '<br />

When w = 0 there are two frequeucies <strong>of</strong> bending vibrations for<br />

forward <strong>and</strong> two for reverse precession.. Since the shaft is<br />

turning there is no gyroscopic moment <strong>and</strong> the frequencies in the<br />

regions <strong>of</strong> forward <strong>and</strong> reverse precession, by pairs, are equal<br />

(in<br />

absolute value).<br />

not<br />

When w > 0 in the region <strong>of</strong> forward precess'ion, the ntimerical<br />

values <strong>of</strong> X are greater than when w = 0, an in the region <strong>of</strong> reverse,<br />

precession are less. This is explained by the effect <strong>of</strong>:the gyroscopic<br />

moment which, during forward precession, increases shaft rigidilty<br />

<strong>and</strong> during reverse decreases it.<br />

; 367

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