UDC 546.732:543.5The temperature dependence of heat capacity of the polycrystalline sample of cobalt(II) clathrochelate in a range of 6-300 K is studied. Based on the smoothed dependence C p (Ɍ), the entropy and enthalpy values in a temperature range of 8-300 K and their standard values at 298.15 K are calculated. In the C p (Ɍ) curve in a range of 50-70 K, a process is recorded whose entropy and enthalpy are 1.2 J(Kmol -1 ) and 68 Jmol -1 respectively. A comparison of the results with the data of a multitemperature X-ray diffraction study makes it possible to attribute this process to the structural phase transition.Unlike aliphatic and aromatic macrobicyclic tris-dioximates of cobalt(II) that are low-spin d 7 complexes due to the high-strength field of the encapsulating ligand, clathrochelate derivatives of dihalogendioximes, according to the data of magnetochemical studies, exhibit a gradual and stepped incomplete spin transition 1/2 l 3/2 typical of Co 2+ complexes (d 7 electronic configuration) [1]. This is explained by significant electronic effects of six strong electron-acceptor substituents in the edge chelating moieties of the highly conjugated polyazomethine cell ligand, which lead to a decrease in the donor capacity of coordinating oxime nitrogen atoms [2]. A previous [1] multitemperature X-ray diffraction study of a single crystal of Co(Cl 2 Gm) 3 (Bn-C 4 H 9 ) 2 clathrochelate (Scheme 1) made it possible both to characterize the structure of the 1/2 l 3/2 spin transition in the crystal of this complex and reveal the structural manifestation of the Jahn-Teller effect, and to establish a structural phase transition in a low temperature region. This work was intended to scrutinize this structural phase transition by X-ray diffraction analysis and calorimetry and to determine its thermodynamic parameters.Experimental. Low-temperature X-ray diffraction studies of a single crystal of Co(Cl 2 Gm) 3 (Bn-C 4 H 9 ) 2 were performed using a Bruker APEX II CCD automated diffractometer equipped with a graphite monochromator (MoK D radiation, O = 0.71073 Å) [3,4]. The absorption was taken into account using the Bruker SADABS software (version 2.10) [5].The structure was solved by a direct method and refined by full-matrix LSM in the anisotropic approximation for non-hydrogen atoms using the SHELXTL software [6]. The sites of hydrogen atoms were identified from the difference Fourier synthesis and refined using the riding model with U iso (H) = nU eq (C), where n = 1.5 for methyl and 1.2 for the other 1 A. V. Nikolaev