The focus of this contribution is the numerical treatment of interface coupled problems concerning the interaction of incompressible fluid flow and permeable, elastic structures. The main emphasis is on extending the range of applicability of available formulations on especially three aspects. These aspects are the incorporation of a more general poroelasticity formulation, the use of the cut finite element method (CutFEM) to allow for large interface motion and topological changes of the fluid domain, and the application of a novel Nitsche-based approach to incorporate the Beavers-Joseph (-Saffmann) tangential interface condition. This last aspect allows one to extend the practicable range of applicability of the proposed formulation down to very low porosities and permeabilities which is important in several examples in application. Different aspects of the presented formulation are analyzed in a numerical example including spatial convergence, the sensitivity of the solution to the Nitsche penalty parameters, varying porosities and permeabilities, and a varying Beavers-Joseph interface model constant. Finally, a numerical example analyzing the fluid induced bending of a poroelastic beam provides evidence of the general applicability of the presented approach.C. Ager et al. / 1-25 2 mechanics model valid for "small" deformation. In the fluid domain, the Stokes equations [3,5,7,8] or, including the effect of convection, the Navier-Stokes equations [4,6] are applied. On the fluid-poroelastic interface, either the Beavers-Joseph-Saffmann [3][4][5]7] or a "no-slip" condition [5,6,8] in tangential interface direction are consulted. Details on these interface conditions for the coupling of fluid and (rigid-)porous flow can be found in [10][11][12][13][14] and the references therein.Motivated by the specific requirements of a fluid-poroelastic interaction (FPI) formulation to model rough surface contact in fluid-structure interaction (as in [2]), we extend the range of applicability of these formulations by several aspects. First, a more general formulation for the poroelastic domain, which is based on the same fundamental physical equations as the classical Biot-system, is applied. This formulation allows one to take into account large deformation and the motion of the poroelastic domain, a wide variety of material models by arbitrary strain energy density functions, and varying deformation dependent porosity (see [15][16][17] for details on this formulation and [18] for fundamentals). Second, in order to allow for large deformation and motion or even topological changes of the fluid domain, a cut finite element method (CutFEM) is applied. Herein, a non-interface-fitted, fixed-grid Eulerian computational mesh for the fluid domain is combined with an interface fitted computational mesh of the poroelastic domain in Lagrangian description w.r.t. the displacements of the poroelastic solid phase. Development of the CutFEM, as it will be applied to fluid equations, started by analyses on the Poisson equation [19], the Stok...