Irrotational flows of a viscous fluid satisfy the Navier-Stokes equations. These flows depend on the Reynolds number Re and reduce to inviscid potential flow when the Reynolds number is infinite. The papers in this collection
show that potential flow at a finite Reynolds number is a rich theory
which yields excellent physical results in selected cases. When
considering potential flow it is neither necessary nor useful to put the
viscosity to zero. The theory of irrotational flow of a viscoelastic
fluid is also a valuable and useful theory for linear viscoelastic
fluids, second order fluids and special solutions of more general
models.
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