“…Let Ω ⊂ ℝ 3 be the open, bounded domain occupied by the fluid-solid mixture, with Lipschitz boundary 𝜕Ω. Motivated by applications in biomechanics (like tissue perfusion [3,15,24,36,38,47]), we work under the assumptions of full saturation, negligible inertia, small deformations and incompressible mixture components (in the sense that the solid and fluid phases can't undergo volume changes at the microscale). Due to the complex composition of biological tissue, which exhibit both elastic and viscoelastic behaviors, we consider both poroelastic and poroviscoelastic systems, where the effective stress tensor is of Kelvin-Voigt type.…”