Euler-Euler fluid models are used in various fields to describe multiphase dispersions. Each fluid in the system fulfils its own balance equations, all of which are interconnected through coupling forces. Among them, nonlinear drag forces play a central role in fluid-fluid and fluid-particle interactions. Fully implicit schemes are often prohibitive, as they force all phase equations into one large, complex, monolithic block. Therefore, extrapolated (time-lagged) drag terms are computationally attractive: they can eliminate costly nonlinearities and interphase couplings. Yet explicit approximations must be carefully designed, lest they lead to unstable energy growth. In this context, the present work proposes simple first- and second-order extrapolations for the drag terms and shows how they preserve desired dissipative properties and unconditional numerical stability. This enables the design of efficient, fully decoupled multiphase solvers without CFL conditions.