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Future Directions in Applied Mathematics
International Conference on the Occasion of
Jean-Claude Nédélec's 60th Birthday
Institut Henri Poincaré
11, rue Pierre et Marie Curie - Paris 5ème
June 18, 19, 20 2003
11:30 AM - Wednesday, June 18, 2003 - Amphitheater Darboux
Thomas Y. Hou
Applied Mathematics, 217-50
Caltech
Pasadena, CA 91125, USA
hou@ama.caltech.edu
Singularity Formation Induced by 3-D Hydrodynamic Instability
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One of the classical examples of hydrodynamic instability occurs when
two fluids are separated by a free surface across which the tangential
velocity has a jump discontinuity. This is called Kelvin-Helmholtz
instability. Kelvin-Helmholtz instability is a fundamental instability
of incompressible fluid flow at high Reynolds number. The idealization
of a shear layered flow as a vortex sheet separating two regions of
potential flow has often been used as a model to study mixing properties,
boundary layers and coherent structures of fluids. It is well known that
small initial perturbations on a vortex sheet may grow rapidly due to
Kelvin-Helmholtz instability. The problem is ill-posed in the Hadamard
sense. Most analytical studies of vortex sheet singularity to date rely
heavily on complexifying the interface variables. It is not clear how
to generalize this technique to 3-D vortex sheets in a natural way.
In a joint work with G. Hu and P. Zhang, we study the singularity formation
of 3-D vortex sheets using a new approach. First, we derive a leading order
approximation to the boundary integral equation governing the 3-D vortex
sheet. This leading order equation captures the most singular contribution
of the integral equation. Moreover, after applying a transformation to the
physical variables, we found that this leading order 3-D vortex sheet
equation de-generates into a two-dimensional vortex sheet equation in the
direction of the tangential velocity jump. This rather surprising result
confirms that the tangential velocity jump is the physical driving force
of the vortex sheet singularities. We show that the singularity type of
the three-dimensional problem is similar to that of the two-dimensional
problem. Moreover, we introduce a generalized Moore's approximation to
3-D vortex sheets. This model equation captures the same singularity
structure of the full 3-D vortex sheet equation, and it can be computed
efficiently using Fast Fourier Transform. This enables us to perform
well-resolved calculations to study the generic type of 3-D vortex sheet
singularities. We will provide detailed numerical results to support the
analytic prediction, and to reveal the generic form of the vortex sheet
singularity.
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