The solution for axisymmetric stagnation point flow in the presence of a solid wall was first obtained by Homann (1936). A typical example of this flow is the forward stagnation point appearing in a flow past a sphere. Paul A. Libby (1974)(1976) extended Homann's work by allowing the solid wall to translate along its own plane with a constant speed and allowing constant suction or injection at the solid surface.  
The solution for this problem is obtained in the cylindrical coordinate system  by introducing
where  is the translational speed of the wall and  is the injection (or, suction) velocity at the wall. The problem is axisymmetric only when . The pressure is given by
The Navier–Stokes equations then reduce to
along with boundary conditions,
When , the classical Homann problem is recovered.