“…To describe the kinematics of the thin-walled preform, we consider the configurations of the solid (preform) and fluid (liquid and air) in Figure 3. The thin-walled preform is considered as a single director shell surface Ω 0 with the normal N. Furthermore, we assume that the preform can compress or expand only along the director N, as discussed in [46]. To measure the deformation, we define the stretch λ as the ratio between the thicknesses of the deformed preform, h, and the undeformed preform, h 0 , i.e.,…”