“…The geometrization of Continuum Mechanics was continued afterwards, under the impulse of Marsden and Hughes [48], and is still alive today [14,72,69,78,77,25,76,36,60,10,18,5,75,70]. The possibility to make mechanical calculations (and numerical discretizations in [19,20]) directly on the body B emerges with the formulation, by Noll [57] and later by Rougée [63], of so-called intrinsic stresses, and by the possibility to recast boundary conditions on the abstract manifold B (see Noll's formulation in [59]). In line with Eringen [15], Green and Zerna [28], Benzecri [3], Noll [57,59], and then Epstein and Segev [14], Rougée [63,65,66,67] has furthermore rightly understood the fundamental role played in Continuum Mechanics by the manifold of Riemannian metrics on the body B.…”