As a fundamental equation in the boundary layer theory, the Prandtl system was
derived by Prandtl in 1904. It describes the behavior of an incompressible viscous flow
near a boundary in a small viscosity limit with non-slip boundary condition. Despite
of its importance in physics, the general well-posedness theories and the justification of
the Prandtl system remain as challenging unsolved problems in mathematics. So far,
there are only a few rigorous mathematical results on the well-posedness theory and
the limit is only justified in the framework of analytic functions locally.In fact, since the classical work by Oleinik and her collaborators in 1960s about the
local well-posedness theories for two space dimensional (2D) Prandtl system, important
progress has been made on the global existence of weak solution, well-posedness
framework for analytic data, instability and ill-posedness theories in Sobolev spaces,
etc. Since Crocco transformation plays an important role in Oleinik's theory but it can
not be applied to the study on the Navier-Stokes equations, recently, we introduced a
direct energy method to study the well-posedness of the 2D Prandtl system in Sobolev
spaces without using the Crocco transformation. Some local in time results have been
obtained. We hope that this approach will shed some light on the three space dimensional
(3D) problem and the justification of the limit from the Navier-Stokes equations
to the superposition of the Prandtl system and the Euler equations.Hence, in this research proposal, we will investigate whether under some conditions,
classical solutions can persist for a long time so that we can study their large time
behavior, or some kind of singularity will eventually form so that the solutions will
blowup in finite time in the setting of Sobolev spaces. Moreover, we will investigate
the 3D Prandtl system. Here, notice that so far the global existence of weak solution in
2D was obtained by Xin-Zhang under a favorable condition on the pressure in addition
to the monotonicity condition on the tangential velocity. Moreover, almost all the
existing mathematical theories are for 2D problems. Hence, the problems proposed
in this project are extremely challenging so that the expected outcome may only be
obtained in some restrictive settings. However, we believe that even a small progress
in these directions will lead to the enrichment of the mathematical theories for the
Prandtl system.