The flow field inside a cylindrical container caused by the impulsively sta
rted constant co-rotation or counter rotation of the top-bottom endwalls wi
th fixed sidewall is described. After a transient phase from an initial sta
te at rest a steady flow situation is reached. The unsteady axisymmetric Na
vier-Stokes equations describing the transient flow are expressed in vortic
ity-stream function form. For large values of Reynolds number (based on ang
ular velocity on the lower endwall) an upwind differencing in the spatial d
erivatives for the convective terms is used. A fourth-order accurate compac
t difference scheme is applied to solve the Poisson equation. The results s
how that the slight co-rotation of the top-bottom endwalls induces a breakd
own bubble at a critical value of the Reynolds number which is much smaller
than the value of the Reynolds number for the onset of Vortex breakdown in
a now due to rotation either of the top or bottom end wall. On the other h
and, a weak counter-rotation of top-bottom endwalls suppresses the vortex b
reakdown. The question of whether the similarity solutions are locally usef
ul in describing the flow between finite disks is also addressed.