Governing equations for the stream function

Now we would like to get the identical answer by using the stream function.  The stream function can always be defined in two-dimensions from the continuity equation and for axisymmetric 3-D flows.  For spherical coordinates, the velocity components are (in terms of ψ)

[Graphics:../Images/inviscid_sphere_gr_50.gif] = [Graphics:../Images/inviscid_sphere_gr_51.gif] [Graphics:../Images/inviscid_sphere_gr_52.gif]   [Graphics:../Images/inviscid_sphere_gr_53.gif] = -[Graphics:../Images/inviscid_sphere_gr_54.gif] [Graphics:../Images/inviscid_sphere_gr_55.gif]

[Graphics:../Images/inviscid_sphere_gr_56.gif]
[Graphics:../Images/inviscid_sphere_gr_57.gif]

To get  the governing equation for ψ, we use our definition obtained from the continuity equation and substitute into the vorticity components.  Inspection of the components reveals that the [Graphics:../Images/inviscid_sphere_gr_58.gif] and [Graphics:../Images/inviscid_sphere_gr_59.gif] ==0 identically, the only interesting component is [Graphics:../Images/inviscid_sphere_gr_60.gif]  (i. e. coordinate φ).  This component is   

[Graphics:../Images/inviscid_sphere_gr_61.gif]
[Graphics:../Images/inviscid_sphere_gr_62.gif]

We can simplify this to be

[Graphics:../Images/inviscid_sphere_gr_63.gif]
[Graphics:../Images/inviscid_sphere_gr_64.gif]

which = 0 if there is no vorticity.  Thus with the restriction of no vorticity, which should not be produced by an inviscid flow, then a simple PDE can be obtained for the stream function.

Note that this is NOT the Laplace equation (It would be for a planar flow!!), even though it looks similar.  Compare to the Laplace equation from above.  

[Graphics:../Images/inviscid_sphere_gr_65.gif]
[Graphics:../Images/inviscid_sphere_gr_66.gif]


Converted by Mathematica      June 18, 2000