“…[5] This is important for modelling impurity dynamics because impurities may be present as a significant fraction of the background plasma species, or, in case of deuterium-tritium plasmas, tritium, being a main ion species, cannot be modelled as trace over an existing deuterium-electron plasma. The Zhdanov closure is already implemented, though only using single-temperature collision coefficients at the plasma common temperature, in SOL/edge simulators such as Soledge3x-EIRENE, [1,6,7] SOLPS, [8][9][10] B2-EIRENE, [11] and EDGE2D. [12] Generally, the depth of the closure is represented by the number of moments, that is, 5N-moment, 13N-moment, 21N-moment, or 29N-moment, where N represents the number of species.…”