In 1978, Murdoch presented a direct second-gradient hyperelastic theory for thin shells in which the strain-energy density associated with a deformation η of a surface S is allowed to depend constitutively on the three kinematical descriptors C, H, and F⊤G, where F=GradSη, C=F⊤F, H=F⊤LS′F is the covariant pullback of the curvature tensor LS′ of the deformed surface S′, and G=GradSF. On the other hand, in Koiter’s direct thin-shell theory, the strain-energy density depends constitutively on only C and H. Due to the popularity of Koiter’s theory, the second-order tensors C and H are well understood and have been extensively characterized. However, the third-order tensor F⊤G in Murdoch’s theory is largely overlooked in the literature. We address this gap, providing a detailed characterization of F⊤G. We show that for η twice continuously differentiable, F⊤G depends solely on C and its surface gradient GradSC and does not depend on LS′. For the special case of a conformal deformation, we find that a suitably defined strain measure corresponding to F⊤G depends only the conformal stretch and its surface gradient. For the further specialized case of an isometric deformation, this strain measure vanishes. An orthogonal decomposition of F⊤G reveals that it belongs to a ten-dimensional subspace of the space of third-order tensors and embodies two independent types of non-local phenomena: one related to the spatial variations in the stretching of S′ and the other to the curvature of S.
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