Volume-averaged Navier--Stokes equations are used in various applications to model systems with two or more interpenetrating phases. Each fluid obeys its own momentum and mass equations, and the phases are typically coupled via drag forces and a shared pressure. Monolithic solvers can therefore be very expensive and difficult to implement. On the other hand, designing robust splitting schemes requires making both pressure and drag forces explicit without sacrificing temporal stability. In this context, we derive a new first-order pressure-correction method based on the incompressibility of the mean velocity field, combined with an explicit treatment of the drag forces. Furthermore, the convective terms are linearised using extrapolated velocities, while the viscous terms are treated semi-implicitly. This gives us an implicit-explicit (IMEX) method that is very robust not only due to its unconditional energy stability, but also because it does not require any type of fixed-point iterations. Each time step involves only linear, scalar transport equations and a single Poisson problem as building blocks, thereby offering both efficiency and simplicity. We rigorously prove temporal stability without any time-step size restrictions, and the theory is confirmed through two-phase numerical examples.
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