 Solution

For Co, the full field-polarized ionic value isThis is distinct from the much smaller weak-ferromagnetic domain moment, approximately 450 G cm${}^3$ mol${}^{-1}$ at low field. A low-temperature isothermal loop should have a small hysteretic central component superposed on the antiferromagnetic field response. Reversal changes the selected weak-ferromagnetic domain and produces remanence and coercivity. At larger fields the magnetization continues to increase as the opposed sublattice moments rotate; a spin-flop or spin-reorientation feature may occur depending on field direction and anisotropy. Only sufficiently strong fields approach the full ionic saturation value, so the small low-field loop must not be labelled as saturation at 4.25 ${\mu }_B$.