We initiate the systematic study of a particularly tractable and physically motivated
hyperpressure constitutive relation for second-gradient incompressible viscous fluids.
As the simplest relation within a broader family, it yields models that are physically
and mathematically attractive. The resulting framework for second-gradient
incompressible viscous fluids with constant viscosity is further extended in a novel
way to incorporate pressure-dependent viscosities. We show that for the
pressure-dependent viscosity model, the inclusion of second-gradient effects and the
constitutive relation for the hyperpressure guarantee the ellipticity of the
governing pressure equation, in contrast to previous models rooted in classical
continuum mechanics. The constant viscosity model is applied to steady
cylindrical flows, where explicit solutions are derived under both strong and weak
adherence boundary conditions. In each case, we establish convergence of
appropriately nondimensionalised velocity profiles to the classical Navier–Stokes
solutions as the model’s characteristic nondimensionalised length scales tend to
zero.