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Report of the Second Piloted Aircraft Flight Control System - Acgsc.org

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Note that d$, is identical to k;', listed in Table I.<br />

SPDG CONSTANTS AND MASSES EQUAL - A large portion <strong>of</strong> <strong>the</strong> foregoing<br />

discussion has to be based upon <strong>the</strong> asmmption that approximate<br />

factorization <strong>of</strong> <strong>the</strong> transfer function dmaxbtor is ssible. This<br />

tacitly aeeumes that <strong>the</strong> ad /-- are considerably<br />

separated, If <strong>the</strong>se quantities are wt separated by a wide<br />

margin, <strong>the</strong>re are no means available to detezmine <strong>the</strong> effect <strong>of</strong> change <strong>of</strong><br />

an individual parameter upon <strong>the</strong> system except by <strong>the</strong> use <strong>of</strong> numerical<br />

values.<br />

It is, however, valuable to investigate a Umiting case where <strong>the</strong><br />

values <strong>of</strong><br />

'<br />

=/M, and are close toge<strong>the</strong>r, <strong>the</strong><br />

case for which Aa/, - 4<br />

=-A' and M= = Ms = M . For<br />

simplification it is also assumed that <strong>the</strong> valve damping,<br />

zero. The open loop transfe~ function <strong>the</strong>n becomes:<br />

8, , is<br />

uhlch, with approximate factors becanes:<br />

The Bode diagram <strong>of</strong> this system is shown in Fig. U),

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