“…The initial core-surface model by Gurtin and Murdoch is an idealized model as it ignores the surface layer thickness and thus describes the surface as a stretchable but not a bendable structure. ,− This approach is further improved by a series of core–shell models, ,, where the NW cross section is considered as a composite structure composed of a bulk core and a surface layer of finite thickness, each with its distinct set of elastic constants. , The definition of the effective bending rigidity is another cause of further discrepancy among nanomechanical models. , The term originates from the local geometric nonlinearity of strains through incremental deformation theory. , Ignoring its dependence on parameters such as surface-induced residual stresses renders YL and modified YL models incapable of capturing surface stress effects emanating from NW side surfaces . These effects are significant upon large deformation of NWs leading to axial reorientations and phase transformations. , Consequently, the effectiveness of available nanomechanical models ,,− in predicting NW bending behavior is directly related to the extent of their parameter sets.…”