Abstract
In [3] ([4]) M. Bartolozzi and Aldo Bressan considered a regular portion Δσ of a m-dim. Riemaniann manifold σ=σ(t), possibly moving in a Euclidean spaceS v and introduced the notion of (volume preserving) velocity fields as rigid as possible—in shortV F R P (V P V F R P)—as an extension of rigid velocity fields —R V F—of classical physics. Existence problems were not considered.
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