For compressible, isotropic, hyperelastic solids, we consider two effects which are absent in
the linear theory but necessarily present (to some extent) in the nonlinear theory, namely, the
dependence of pressure on shear strain and the dependence of shear stress on volumetric strain.
Typically, only limited experimental data is available on these nonlinear effects, so it is
common to make some simplifying assumptions on their functional form. However, some care must be
taken here since the dependence of pressure on shear strain and the dependence of shear stress
on volumetric strain are coupled through the strain energy function. For example, it is often
assumed that the pressure is independent of the shear strain or that the shear stress is
independent of the volumetric strain. While neither one of these assumptions individually
violates the existence of a strain energy function, both assumptions taken together are
inconsistent with the existence of a strain energy function. The problem that will be addressed
is to determine the most general form of the strain energy function compatible with various
assumed forms of the dependence of pressure on shear strain, and consequently to determine the
restrictions imposed on the dependence of shear stress on volumetric strain, or vice versa.
Since experimental data on the latter effect is often reported as a dependence of shear stress
on pressure, we also consider the consequences of various simplifying assumptions for this
dependence. Several known results are recovered as special cases.
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