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

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tp = 4 1' ( 4 include. aU flaxibillty I- <strong>the</strong><br />

a! hydraulic cylinder to <strong>the</strong> effective mass<br />

cmter <strong>of</strong> <strong>the</strong> surface)<br />

A' = surface horn radius<br />

d = surface span<br />

<strong>the</strong>n in meal terms, equation (51) becomes:<br />

Caparison <strong>of</strong> equation (52) with (49) clearly sbua that <strong>the</strong> camplete<br />

apresrion for <strong>the</strong> hgdraulic-flutter sfst- is far more oarpl~x than<br />

<strong>the</strong> rimple situation shown in Pig, l4.<br />

The above ca~~ponant <strong>of</strong> <strong>the</strong> total aerodyneaic =ant nlatsd to<br />

and its derivatives ahe now replaces <strong>the</strong> orfginal incamplets tern<br />

in equation (50); <strong>the</strong>nfore <strong>the</strong> differential equation <strong>of</strong> motion ir more<br />

precisely ~3q)ressed,<br />

p diagraa~at$c reprermtath <strong>of</strong> <strong>the</strong> corrdcted capansnt ir ram .<br />

in Fig. 16.

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