Corrigendum to “Shear wave propagation in finitely deformed 3D fiber-reinforced composites” [Int. J. Solids Struct. 110–111 (2017) 294–304] (S0020768316303742) (10.1016/j.ijsolstr.2016.12.007))

In our paper (Galich et al., 2017), Figs. 7–9 show frequencies as functions of wavenumber K⁰ (in the undeformed configuration); thus, in Figs. 7–9, [Formula presented] must replace [Formula presented] (in the deformed configuration). Recall that the corresponding wave vectors in the undeformed and deformed configurations are related via [Formula presented]. Here, we present frequencies as functions of wavenumber k in the deformed configuration. Figs. 1 –3 correspond to Figs. 7, 8 and 9, respectively, in the original paper (Galich et al., 2017). Thus, the conclusion in Galich et al. (2017) about the weak influence of the applied deformation on short shear waves (with wavelength l ≲ 2a) needs to be corrected. As can be seen from Fig. 2, the applied uniaxial deformation influence shear waves in both long and short wave ranges. All other conclusions in Galich et al. (2017) agree with the dispersion curves presented in Figs. 1–3.