This　paper　is　concerned　with　the　bipolar　compressible　Navier-Stokes-Maxwell　system　for　plasmas.　We　investigated,　by　means　of　the　techniques　of　symmetrizer　and　elaborate　energy　method,　the　Cauchy　problem　in　R-3.　Under　the　assumption　that　the　initial　values　are　close　to　a　equilibrium　solutions,　we　prove　that　the　smooth　solutions　of　this　problem　converge　to　a　steady　state　as　the　time　goes　to　the　infinity.　It　is　shown　that　the　difference　of　densities　of　two　carriers　converge　to　the　equilibrium　states　with　the　norm　parallel　to.parallel　to(Hs-1),　while　the　velocities　and　the　electromagnetic　fields　converge　to　the　equilibrium　states　with　weaker　norms　than　parallel　to.parallel　to(Hs-1).　This　phenomenon　on　the　charge　transport　shows　the　essential　difference　between　the　unipolar　Navier-Stokes-Maxwell　and　the　bipolar　Navier-Stokes-Maxwell　system.