Unformatted text preview: y d A 2 x d 2 x a 2 y c 2 y d 2 x b 2 x c 2 y a 2 y b 2 Γ 1 2 0.3 1 s 2 2 1 2 2 2 1 2 1 2 2 2 1 2 2 2 m 2 Γ m 2 s This result is to be expected since the flow is irrotational and by Stokes' theorem, the circulation is equal to the curl of the velocity over the bounded area (Eqn. 5.18)....
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 Fall '07
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 Fluid Mechanics, Vector Calculus, Vector field, Stokes' theorem, velocity field

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