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A Survey of Unsteady Hypersonic Flow Problems

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a<br />

a,<br />

A<br />

b<br />

c<br />

cD<br />

CL<br />

%l<br />

%I<br />

c%<br />

C Q%<br />

C mq<br />

C P<br />

d<br />

E<br />

Ez<br />

f<br />

fi<br />

- 62 -<br />

Nomenclature<br />

(Some terms are not included III this index if<br />

they are used only locally)<br />

local speed <strong>of</strong> sound<br />

free-stream value <strong>of</strong> speed <strong>of</strong> sound<br />

aspect ratlo <strong>of</strong> wing (span/mean chord)<br />

representative length <strong>of</strong> a body($ for a wing, 8 for a body)<br />

mean chord <strong>of</strong> a wing<br />

drag coefficient <strong>of</strong> a body [Drag&@S]<br />

lift coefficient <strong>of</strong> a body [Lift/&U'S]<br />

rate <strong>of</strong> change <strong>of</strong> lift coefficient with angle <strong>of</strong> attack: X+/&x<br />

pitching moment coefficient<br />

rate <strong>of</strong> change <strong>of</strong> pitching moment coefficient with angle <strong>of</strong><br />

attack: acdaa<br />

rate <strong>of</strong> change <strong>of</strong> pitching moment coefflczsnt with time<br />

irb %I<br />

rate <strong>of</strong> change <strong>of</strong> angle <strong>of</strong> attack parameter, - :<br />

U eoJ)<br />

rate <strong>of</strong> change <strong>of</strong> pitching moment ccefflclent with pitching<br />

Ob a%<br />

velocity parameter, - :<br />

IJ a(db/b)<br />

pressure coefflcvent<br />

maximum body diameter<br />

Young's Modulus<br />

P - P,<br />

&JJ"<br />

effective stiffness based on frequency <strong>of</strong> second elastic mode<br />

frequency <strong>of</strong> oscillation<br />

frequency <strong>of</strong> natural mode : i = 1 for first mode, etc.<br />

gravitational constant<br />

structural damping factor<br />

altitude

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