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CDS/CIMMS Lunchtime Seminar: Swimming of a Deformable Body due to Transverse Shape Deformations

Dr. Eva Kanso, Department of Aerospace and Mechancial Engineering, University of Southern California

Thursday, February 21, 2008
12:00 PM to 1:30 PM
Steele 114 (CDS Library)

The net locomotion of a deformable body submerged in an infinite volume of fluid depends critically on the dynamic coupling between the prescribed shape deformations and the unsteady motion of the surrounding fluid. A mathematical description of this coupling at finite Reynolds numbers would require taking into account the detailed effects of viscosity which are primarily manifested in the dynamics of the thin shear layers around the body that separate at the body tail to create vortical structures. The classical studies of Wu and Lighthill addressed this problem in two different ways. Wu considered a planar deformable plate swimming in an inviscid fluid and used the assumption of small shape amplitudes which enables one to solve for the trailing vortex sheet analytically and investigate the problem of optimum shape deformations in the sense of minimizing the energy lost in creating the trailing wake. Lighthill, on the other hand, studied the swimming of a slender body due to large amplitude deformations and avoided solving for the complex wake dynamics by considering the momentum balance in a control volume containing the deformable body and bounded by a plane attached at its trailing edge.

In this talk, we present a derivation of the laws governing the swimming of a deformable body in response to prescribed (actively controlled) shape deformations and the effect of the wake vorticity. The underlying balance of momenta, though classical in nature,  provide a unifying framework for the swimming of planar and  three-dimensional bodies and they hold even in the presence of viscosity. When applied to the swimming of slender bodies, the derived equations can be viewed as a generalization of Lighthill's slender body theory. When neglecting vorticity, the derived equations reduce to a known model for the locomotion of an articulated body in potential flow. We examine locomotion in potential flow through a number of examples. More precisely, we consider two types of large amplitude deformations: undulatory motion and flapping. We compute the gaits due to both types of shape changes and investigate optimal deformations for the corresponding body geometries.

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