We study in this article a stochastic 3D globally modified Allen-Cahn-Navier-Stokes model in a bounded domain. We prove the existence and uniqueness of a strong solutions. The proof relies on a Galerkin approximation, as well as some compactness results. Furthermore, we discuss the relation between the stochastic 3D globally modified Allen-Cahn-Navier-Stokes equations and the stochastic 3D Allen-Cahn-Navier-Stokes equations, by proving a convergence theorem. More precisely, as a parameter N tends to infinity, a subsequence of solutions of the stochastic 3D globally modified Allen-Cahn-Navier-Stokes equations converges to a weak martingale solution of the stochastic 3D Allen-Cahn-Navier-Stokes equations.2010 Mathematics Subject Classification. 35R60, 35Q35, 60H15, 76M35, 86A05. 395 396 THEODORE TACHIM MEDJOinfancy as noted in [18]. As noted in [17], the mathematical analysis of binary fluid flows is far from being well understood. For instance, the spinodal decomposition under shear consists of a two-stage evolution of a homogeneous initial mixture: a phase separation stage in which some macroscopic patterns appear, then a shear stage in which these patters organize themselves into parallel layers (see, e.g. [26] for experimental snapshots). This model has to take into account the chemical interactions between the two phases at the interface, achieved using a Cahn-Hilliard approach, as well as the hydrodynamic properties of the mixture (e.g., in the shear case), for which a Navier-Stokes equations with surface tension terms acting at the interface are needed. When the two fluids have the same constant density, the temperature differences are negligible and the diffuse interface between the two phases has a small but non-zero thickness, a well-known model is the so-called "Model H" (cf. [21]). This is a system of equations where an incompressible Navier-Stokes equation for the (mean) velocity v is coupled with a convective Cahn-Hilliard equation for the order parameter φ, which represents the relative concentration of one of the fluids.Many challenges in the mathematical and numerical analysis of the Allen-Cahn-Navier-Stokes equations (AC-NSE) or the Cahn-Hilliard-Navier-Stokes equations (CH-NSE) are related to the fact that the full mathematical theory for the 3D Navier-Stokes equation (NSE) is still lacking at present. Since the uniqueness theorem for the global weak solutions (or the global existence of strong solutions) of the initial-value problem of the 3D Navier-Stokes system is not proved yet, the known theory of global attractors of infinite dimensional dynamical systems is not applicable to the 3D Navier-Stokes system. This situation is the same for the 3D coupled Allen-Cahn-Navier-Stokes systems. Using regular approximation equations to study the classical 3D Navier-Stokes systems has become an effective tool both from the numerical and the theoretical point of views. As noted in [38], it was demonstrated analytically and numerically in many works that the LANS-α model gives a good approximation in the s...