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_56.gif]](../Images/inviscid_sphere_gr_56.gif)
![[Graphics:../Images/inviscid_sphere_gr_57.gif]](../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
and
==0 identically, the only interesting component is
(i. e. coordinate φ). This component is
![[Graphics:../Images/inviscid_sphere_gr_61.gif]](../Images/inviscid_sphere_gr_61.gif)
We can simplify this to be
![[Graphics:../Images/inviscid_sphere_gr_63.gif]](../Images/inviscid_sphere_gr_63.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]](../Images/inviscid_sphere_gr_65.gif)