Abstract
Qualitative aspects of mathematical models for the dynamics of liquids with a moving
boundary are studied. These models describe for instance groundwater flow, extraction
of oil, the growth of tumours and viscous sintering in the production of glass.
Stability of radially symmetric solutions and decay properties of perturbations are
studied for the case that in a single point fluid is injected or extracted. For the motion
of the moving boundary a nonlinear non-local evolution equation is derived. The domain
is rescaled in such a way that the spherical solution is represented by a stationary
solution. Because of this rescaling, the evolution operator is time dependent. The nonlinear
stability results are based on linearisation, energy estimates and the principle of
linearised stability.
The Hele-Shaw model is studied for several boundary conditions, describing various
physical situations. In the case of zero pressure on the boundary, it is proved for the
injection problem that balls around the injection point are asymptotically stable with
respect to small star-shaped perturbations. If surface tension regularisation is included,
then balls are stable even for the case of suction under additional assumptions on the
initial geometry, suction speed and dimension. Moreover, perturbations turn out to
decay algebraically fast.
For two dimensional suction, the influence of surface tension dominates the influence
of the sink for large time. As a consequence, no condition on the suction speed is
necessary. In contrast to the two dimensional problem there is a bound on the suction
speed for the 3D problem. In dimensions higher or equal to four the influence of the
sink dominates the influence of surface tension. This leads to linear instability for the
spherical solution for any suction speed.
Making use of the autonomous character of the evolution equation, existence of nontrivial
self-similarly vanishing solutions to the three dimensional suction problem with
surface tension is proved. These solutions are found as bifurcation solutions from the
trivial spherical solution. The suction speed plays the role of bifurcation parameter.
Moreover, one branch of bifurcation solutions turns out to be stable with respect to a
certain class of perturbations.
For the closely related Stokes flow stability of the spherical solution in the case of
injection has been proved for dimensions two and three. For the suction problem for
these dimensions the spherical solution is linearly unstable.
| Original language | English |
|---|---|
| Qualification | Doctor of Philosophy |
| Awarding Institution |
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| Supervisors/Advisors |
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| Award date | 10 Jun 2009 |
| Place of Publication | Eindhoven |
| Publisher | |
| Print ISBNs | 978-90-386-1822-7 |
| DOIs | |
| Publication status | Published - 2009 |
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