  Furukawa predicted that at late times, the domain growth in binary fluids
scales as $\ell(t)\sim t^{2/3}$, and the growth is driven by fluid inertia. The
{\it inertial growth regime} has been highly elusive in molecular dynamics (MD)
simulations. We perform coarsening studies of the Stockmayer (SM) model
comprising of magnetic dipoles that interact via long-range dipolar
interactions as well as the usual Lennard-Jones (LJ) potential. This
fascinating polar fluid exhibits a gas-liquid phase coexistence, and magnetic
order even in the absence of an external field. From comprehensive MD
simulations, we observe the inertial scaling [$\ell(t)\sim t^{2/3}$] in the SM
fluid for an extended time window. Intriguingly, the fluid inertia is
overwhelming from the outset - our simulations do not show the early diffusive
regime [$\ell(t)\sim t^{1/3}$] and the intermediate viscous regime
[$\ell(t)\sim t$] prevalent in LJ fluids.
