Sufficient conditions for inseparability of mixed states include (logarithmic) negativity. Here we explore systems with a globally conserved charge, such as a particle number. We argue that separable states contain entanglement in fixed charge sectors as long as the state can not be separated into symmetric classical components. As a witness of symmetric inseparability we study the entropy change due to a subsystem's charge measurement, ∆Sm. Whenever ∆Sm > 0, there exist inseparable charge sectors, having finite negativity, even when the full state is either separable or has vanishing negativity. We study the scaling of ∆Sm in thermal 1D systems combining high temperature expansion and conformal field theory. We discuss routes towards experimental observation.