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Xy qeog f. X y V x y ds xx J I D D S f ¦. • This allows us to calculate the output g(t) with an input f(t)!. U O M ¨.
Q } V u t v Ò. D – angle of attack;. = , d s s v &.
W M z Ø. S j – length of jth panel;. (7) where ( ) ( ) 1 j j j j j j s s S J J J J (8) in which Vf – velocity of uniform flow, in this article, = 1 m/s;.
, d Q ­. K u y ³. F X y t y é.
Sj – distance measured from the leading edge of the panel;. § 5229Òulesándòegulationsæor€!m,åtc Chapt•H7 ÍISSINGÃHILDRENÉNFORMATIONÃLEAR€ðHOUSE Œy W¾Ði¿Ùmµ;Œ‡š ¾ ¾ ¾ ¾ 03½§½§½§½. 6 W M Ö.
M – vortex panel numbers)xy jj – arbitrary point on the jth panel;. C g d } ¦. 5229Òulesándòegulationsæor€!m,åtc Chapt•H7 ISSINGÃHILDRENNFORMATIONÃLEAR€ðHOUSE Œy W¾i¿Ùmµ;Œ‡š ¾.
O x d } à. Prof Gabriel Popescu Fourier Optics 22 Shift invariance •For linear shift invariant (LSI) systems, the response to a shifted impulse is the shifted impulse response • This means the shape of the impulse response is time independent!.

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