Abstract
According to Stewartson (1969, 1974) and to Messiter (1970), the flow near the trailing edge of a flat plate has a limit structure for Reynolds number
Re
→∞ consisting of three layers over a distance
O
(Re
-3/8
) from the trailing edge: the inner layer of thickness
O
(
Re
-5/8
) in which the usual boundary layer equations apply; an intermediate layer of thickness
O
(
Re
-1/2
) in which simplified inviscid equations hold, and the outer layer of thickness
O
(
Re
-3/8
) in which the full inviscid equations hold. These asymptotic equations have been solved numerically by means of a Cauchy-integral algorithm for the outer layer and a modified Crank-Nicholson boundary layer program for the displacement-thickness interaction between the layers. Results of the computation compare well with experimental data of Janour and with numerical solutions of the Navier-Stokes equations by Dennis & Chang (1969) and Dennis & Dunwoody (1966).
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