Plane-polarised finite-amplitude shear waves in deformed incompressible materials

Abstract

We investigate how two finite-amplitude, transverse, plane body waves may be superposed to propagate in a deformed hyperelastic incompressible solid. We find that the equations of motion reduce to a well-determined system of partial differential equations, making the motion controllable for all solids. We find that in deformed Mooney-Rivlin materials, they may travel along any direction and be polarised along any transverse direction, an extension of a result by Boulanger and Hayes [Quart. J. Mech. Appl. Math. 45 (1992) 575]. Furthermore, their motion is governed by a linear system of partial differential equations, making the Mooney-Rivlin special in that respect. We select another model to show that for other materials, the equations are nonlinear. We use asymptotic equations to reveal the onset of nonlinearity for the waves, paying particular attention to how close the propagation direction is to the principal axes of pre-deformation.

References in corpus (4)

• Finite amplitude elastic waves propagating in compressible solids
• Nonlinear transverse waves in deformed dispersive solids
• Strain energy function for isotropic non-linear elastic incompressible solids with linear finite strain response in shear and torsion
• On the Mathematical and Geometrical Structure of the Determining Equations for Shear Waves in Nonlinear Isotropic Incompressible Elastodynamics