Thermal studies on CuCr204 spinel indicated the phase present above 870 K to be cubic CuCr~O~. However, when the substance was quenched from 1023 K, 1173 K, 1273 K and 1473 K, only the tetragonal phase of CuCr204 was obtained. This is because the first-order, diffusionless, tetragonal to cubic phase transition at 865 K occurs reversibly at a very fast rate. The c/a ratio for CuCr204 present in the various quenched samples did not change when the quenching temperature was raised. A strong preference of the Cr ~+ ion for the B site prevents it from interchanging sites with Cu z* ions, thus keeping the lattice parameters c and a unchanged.Copper(II) chromite (CuCr~O4) and copper(II) ferrite (CuFe~Oa) are tetragonally distorted spinels with c]a < 1 and c]a > 1, and the transition to the cubic form occurs at 873 K and 633 K, respectively [1][2][3][4]. The distortion in these spinels is due to the Cu 2+ Jahn-Teller ion [5,6]. Cr ~+ and Cu e+ both have a strong preference for octahedral coordination, but the former has a comparatively higher octahedral site preference energy [7] and so Cu[Cr2]O4 is a normal spinel, whereas Fe[CuFe]O4 is almost an inverse spinel. However, the degree of inversion of CuFe~O4 changes at higher temperatures, due to a change in the cation distribution, as indicated by the c/a values of CuFe2Oa quenched from various temperatures, and cubic CuFe204 can be obtained by quenching from above 1033 K [4]. Such changes in cation distribution at higher temperatures may also be expected in CuCr204 and the present work is an attempt to study the thermal effect on the cation distribution of CuCr~O~, and the preparation of quenched cubic CuCr204.