In　the　present　paper,　the　full　compressible　Navier-Stokes-Maxwell　equations　are　investigated　in　R-3　and　the　large-time　behavior　of　global　smooth　solutions　is　established.　It　is　shown　that　both　the　density　and　the　temperature　converge　to　the　equilibrium　states　with　the　same　norm　parallel　to　center　dot　parallel　to(Hs-1),　while　the　other　unknown　variables　converge　to　the　equilibrium　states　with　weaker　norms　than　parallel　to　center　dot　parallel　to(Hs-1).　This　phenomenon　on　the　charge　transport　shows　the　essential　difference　of　the　equations　with　the　non-isentropic　Euler-Maxwell　and　the　isentropic　Navier-Stokes-Maxwell　equations.　(C)　2014　Elsevier　Ltd.　All　rights　reserved.