DSC Investigations of the CuO-BaO System Z. Zivkovic1*, N. Strbac1, D. Zivkovic1, D. Grujicic2 'University of Belgrade, Technical Faculty VJ 12, 19210 Bor, Serbia and Montenegro; *Phone/Fax: ++381 30 424 547; E-mail: jmm@eunet.yu PUniversity of Idaho, Department of Materials, Metallurgical, Mining and Geological Engineering, Moscow, USA Abstract: Numerous data obtained by methods of thermal analysis are of the great importance for the determination and identification of the superconducting phases in the system Y-Ba-Cu-O. As a contribution, results of DSC investigations in the copper-based oxide CuO-BaO are presented in this work. Dependencies of specific heat on temperature are determined and values for heat effects at characteristic temperatures are given for investigated binary systems. Keywords: thermal analysis, DSC, CuO-BaO system, superconductors Received: December 14, 2004 Accepted: September IS, 2005 Introduction Discovery of the high-temperature superconducting oxide ceramics in the middle eighties announced the beginning of a new era in the materials science, as well as in many different areas of high-temperature superconductors application. All this lead to increased scientific activity, aimed at characterization of these materials and development of new materials with similar or even better characteristics [1]. Especially, the discovery of superconductivity in the system Y-Ba-Cu-0 has triggered a great interest in the copper-based oxides [1,2]. One of these activities is focused on thermal properties research of these ceramic materials, for they can provide a substantial insight into the theoretical aspect of superconducting transitions [2_4]. Considering the specific heat measurements and heat effects values determination, the literature data are numerous: Costa et al. [3,5] measured heat capacities of the high Tc superconductor YBa2Cu307_g by calorimetric measurements performed in a computer controlled continuous heating adiabatic calorimeter; Kishi et al. [6] investigated the specific heat anomaly of high Tc superconducting ceramics by AC calorimetry, while Niinisto and Karppinen [7] and Zivkovic et al. [8] presented experimental results obtained by DTA and DSC for the study of the YBa2Cu307_g superconductor. Since a larger number of works in this field is done on the superconducting phase YBa2Cu307_g, we focused our research on DSC investigations of the copper-based oxide of Cu0-Ba0 type as one of the main constituents of high-temperature superconducting Y-Ba-Cu-0 ceramics. 470 ZlVKOVIC, Z. ET AL. Experimental DSC technique was used in the experimental investigation of the CuO-BaO system. All experiments were performed on DSC 404 apparatus, by NETZCH, Germany. Samples were synthesized by solid phase sintering of CuO and BaCOQ, in an oxygen atmosphere. Sample mass was 5mg. The samples were placed in Al2O3 crucibles. Sapphire was used as a standard for c evaluation. p Results and Discussion Composition of the investigated samples in the system CuO-BaO are presented in Table I. Results obtained by DSC measuring in the temperature interval up to 1000 °C, which include dependencies of specific heat on temperature and determined values for heat effects at characteristic temperatures, are given in Fig.1. Table I. Composition of the investigated samples in CuO-BaO system. Sample %wt CuO %wt BaO XCuO XBaO 1 20 80 0.32 0.68 2 40 60 0.56 0.44 3 60 40 0.74 0.26 4 80 20 0.89 0.11 First, endothermic peak occurs in the temperature interval 810-812 °C and the enthalpy value is relatively constant. This can be explained by the phase transformation of BaCOQ, used in the preparation of mixture, from rhombic to hexagonal structure. Endothermic peaks at higher temperatures, in the interval 920-935 °C, should be considered together with the known phase diagram of the investigated CuO-BaO system [9] (Fig. 2). According to the literature data c10-12], eutectic line between barium cuprate and CuO is not yet fully estimated. Wong et al. [10] determined the eutectic slightly above 900 °C at about xD = 0.38, while Nevriva et al. [11] BaO ' and Licci et al. [12] found the eutectic point at 925 °C with xBaO = 0.28. Having these facts in mind, one can conclude that endothermic peaks at higher temperatures obtained in this work by using the DSC technique, correspond to the eutectic line in the CuO-BaO system, while the dicsrepancy between reported values and our results can possibly be caused by various materials used as sample holder, presumably due to the formation of an intermediate phase Ba4PtOT [11]. Furthermore, the enthalpy dependencies on the composition, given in Fig. 3, show that the maximal enthalpy value corresponds to the eutectic composition. Moving left or right related to this value show on the enthalpy value decreasing, because of the less quantity of melted phase. Figure I. DSC and specific heat dependencies on temperature for investigated samples CuO-BaO (a - 20 % wt CuO; b - 40 % wt CuO; c - 60 % wt CuO; d - 80 % wt CuO) 472 Žlvkovic, Ž. et al. 8- T503 Li*iJ / / Î S / CuO V «73 1239 Mole fraction of CuO MULE FWCICNOf" Cu %wt. of CuO 60 80 10 a) Phase diagram according to l9] Figure 2. CuO-BaO phase diagram. b) Part of the phase diagram confirmed by DSC ex periments in this work 120" 100 OJ T 80- 20-o- 0 10 20 30 40 50 60 70 80 90 100 %wt. CuO Figure 3. Enthalpy dependence on composition. The analysis of cp variation with temperature and composition, shown in Figure 4., also confirmed mentioned assumption, because a peak on the curve is noted at the eutectic temperature and composition. Figure 4. Specific heat dependence on composition. So, the obtained DSC results for the CuO-BaO system gave us not only the values of the specific heat and enthalpies of the characteristic peaks, but can also be used in the interpretation of the CuO-BaO phase diagram, in the investigated temperature interval up to 1000 °C. Acknowledgement The authors express their thanks to Prof. Jaroslav Sestak, Institute for Physics, Czech Academy of Sciences (Prague, Czech Republic) for his help and recommendations. References [I] Sestak, J. (1989): Thermochim. Acta 148, pp. 235- 248. ra Bednorz, J.G., Muller, K.A. (1986): Z. Phys. 64B, p. 189. Costa, G.A., Ferretti, M., Olcese, G.L. (1988): Thermochim. Acta 137, pp. 65-70. [R] Nevitt, M.V., Crabtree, G.W., Klippert, T.E. (1987): Phys. Rev. 36B, pp. 2398-2400. [5] Costa, G.A., Ferretti, M., Fornasini, M.L., Giordans, M., Olcese, G.L. (1988): Thermochim. Acta, 133, pp. 49-54. [6] Kishi, A., Kato, R., Azumi, T., Okamoto, H., Maesono, A., Ishikawa, M., Hatta, I., Ikushima, A. (1988): Thermochim. Acta 133, pp. 39-42. [7] Niinisto, L., Karppinen, M. (1989): J.Therm. Anal. 35, pp. 319-327. ™ Zivkovic, Z., Zivkovic, D., Strbac, N. (1992): Mining and Metallurgy Quarterly 39(1-2), pp. 6982. P] Lee, B.J., Lee, D.N. (1989): J. Am. Ceram. Soc. 72(2), pp. 314-319. ™ Wong-Ng, W.K., Davis, K.L., Roth, R.S. (1988): J. Am. Ceram. Soc. 71, p. 64. [II] Nevriva, M., Pollert, E., Mateikova, L., Triska, A. (1988): J. Crystal Growth 91, p. 434. ™ Licci, F., Scheel, H.J., Besagni, T. (1988): Physica C 153-155, pp. 431.