“…Returning to the extension-bending-torsion problem (P 1 ) for cylindrical Cosserat shells, we mention that in the isotropic case the constants a 3 , a α and a 4 which satisfy the system (20) can be interpreted as the global measures of axial strain, axial curvature and twist, respectively (see [3]). Suggested by (20), we consider the following problem: to define the functionals τ k (•), k = 1, ..., 4, on the set of solutions…”