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Velocity potential

if u and w can be expressed as the partial derivatives of a function tex2html_wrap_inline1012 ,

i.e. :   ( tex2html_wrap_inline1012 = velocity potential)

eqnarray252

Then the irrotationality condition is satisfied automatically, since:

eqnarray259

In order for the continuity equation to be satisfied we must have:

eqnarray273

Once the velocity potential tex2html_wrap_inline1012 is determined, the whole velocity field is known:

eqnarray284

Definition of tex2html_wrap_inline1018 (also gradient of tex2html_wrap_inline1012 )

So: The goal is to find the velocity potential, tex2html_wrap_inline1012 , which satisfies Laplace equation.



Soon Woong Chang
Thu Sep 23 16:47:16 CDT 1999