== Boundary Layer for Flow Past a Wedge ==
The Blausius boundary layer velocity solution is a special case of a larger class of problems for [http://en.wikipedia.org/wiki/Blasius_boundary_layer flow over a wedge], as shown in the following figure. The angle represents the wedge angle.
[[Image(wedge_bl.png)]]
The general solution is called the Falkner-Skan boundary layer solution, which starts with a recognition that the free-stream velocity will accelerate for non-zero values of :
where is a characteristic length and ''m'' is a dimensionless constant that depends on :
The condition ''m = 0'' gives zero flow acceleration corresponding to the Blausius solution for flat-plate flow.
We then define a similarity variable that combines the local streamwise and cross-flow coordinates ''x'' and ''y'' (defined relative to the surface of the wedge):
Then, defining a function ''f'' that relates to the streamwise and cross-flow velocities, a single ordinary differential equation ensues from boundary layer momentum and mass conservation:
This non-linear equation is not amenable to an exact solution (even for the Blausius solution , which eliminates the last term on the right side). The [http://demonstrations.wolfram.com/NumericalSolutionOfTheFalknerSkanEquationForVariousWedgeAngl/ following Mathematic CDF file] solves the equation numerically and provides the streamwise velocity normalized by the local freestream velocity as a function of .
=== CDF Tool [[FootNote("Numerical Solution of the Falkner-Skan Equation for Various Wedge Angles" from the Wolfram Demonstrations Project
http://demonstrations.wolfram.com/NumericalSolutionOfTheFalknerSkanEquationForVariousWedgeAngl/)]] ===
[[File(NumericalSolutionOfTheFalknerSkanEquationForVariousWedgeAngl.cdf)]]