The isomorphous structures of M(tcm) 2 [M II = Cr, Mn, Fe, Co, Ni, Cu, Zn, Cd or Hg; tcm Ϫ = tricyanomethanide, C(CN) 3 Ϫ ] contain two interpenetrating rutile-related networks generated by octahedral six-connecting metal ions and trigonal three-connecting tcm Ϫ anions. The detailed variable temperature and variable field magnetic properties of this series of high-spin complexes generally point to the existence of very weak intraframework coupling with no evidence for long range magnetic order or interframework effects. The compound Cr(tcm) 2 is the most strongly coupled and displays a field independent maximum in susceptibility at 14.5 K and a J value of Ϫ1.6 cm Ϫ1 (using a Ϫ2JS 1 ؒS 2 Heisenberg chain model); Co(tcm) 2 displays high temperature magnetic moments typical of essentially uncoupled octahedral centres but with a most unusual field dependence in µ Co observed below 10 K, probably due to very weak ferromagnetic coupling, and an M sat value in high fields, at 2 K, which is significantly less than that expected for S = 3/2. Doping of M(tcm) 2 with another MЈ member of the series leads to a crystal structure isomorphous with M(tcm) 2 in which the dopant metal MЈ occupies the M site in a random fashion. The resultant magnetism is simply intermediate between those of the parent phases. The isomorphous structures of [M(tcm) 2 (EtOH) 2 ] (M II = Co or Ni) contain pseudo square-grid sheets in which the tcm Ϫ ligands are each co-ordinated to two metal ions and act as a kinked bridge. Each metal is co-ordinated to four tcm Ϫ anions in an equatorial arrangement and to two axial ethanol ligands. Extensive intrasheet hydrogen bonding exists between the ethanol molecules and the unco-ordinated nitrile of the tcm Ϫ bridges.