== Boundary Layer for Flow Past a Wedge == The Blausius boundary layer velocity solution is a special case of a larger class of problems for flow over a wedge, as shown in the following figure. The angle \beta \pi 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 \beta: u_{e}(x)= U_{0} \left( x/L \right) ^{m} where L is a characteristic length and ''m'' is a dimensionless constant that depends on \beta {\beta} = \frac{2m}{m + 1} The condition ''m = 0'' gives zero flow acceleration corresponding to the Blausius solution for flat-plate flow.