A stationary incompressible Stokes flow in a sphere is considered. The
flow was introduced by Stone et al, (1991) as a flow inside a neutral
ly buoyant spherical drop immersed in a linear flow, The velocity fiel
d of the how is a result of a small perturbation of an integrable velo
city field with almost all streamlines closed, Under arbitrarily small
perturbation a large domain of chaotic advection within the sphere ar
ises. This phenomenon is explained by quasirandom changes in the adiab
atic invariant of the flow, which occur as a streamline crosses the tw
o-dimensional separatrix of the unperturbed flow. Phase portraits of t
he averaged system are constructed. An asymptotic formula for the chan
ge in the adiabatic invariant due to the separatrix crossing is derive
d. The process of diffusion of the adiabatic invariant due to multiple
separatrix crossings is described.