“…Here Ω is the domain occupied by the fluid, Γ denotes the boundary of Ω, v is the velocity, S is the extra-stress tensor, p is the pressure, f denotes the body force, E is the elastic part of the extra-stress tensor, D(v) is the strain-rate tensor, D(v) = 1 2 ∇v + (∇v) T , the operator D ρ /Dt is the regularized Jaumann derivative [42]. In the stationary case, this operator is defined by the formula…”