The subject of so-called objective derivatives in Continuum Mechanics has
along history and has generated varying views concerning their true
mathematical interpretation. Several attempts have been made to provide a
mathematical definition that would at least partially unify the existing
notions. In this paper, we demonstrate that, under natural assumptions, all
objective derivatives correspond to covariant derivatives on the
infinite-dimensional manifold Met(B) of Riemannian metrics on the body.
Furthermore, a natural Leibniz rule enables canonical extensions from covariant
to contravariant tensor fields and vice versa. This makes the sometimes-used
distinction between objective derivatives of Lie type'' and corotational
type’’ unnecessary. For an exhaustive list of objective derivatives found in
the literature, we exhibit the corresponding covariant derivative on Met(B).

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