S. Mukhopadhyay et Kt. Jacob, PHASE-EQUILIBRIA IN THE SYSTEM NIO-CAO-SIO2 AND GIBBS ENERGY OF FORMATION OF CANISI2O6, Metallurgical and materials transactions. A, Physical metallurgy andmaterials science, 26(9), 1995, pp. 2311-2315
Phase relations in the pseudoternary system NiO-CaO-SiO2 at 1373 K are
established. The coexisting phases are identified by X-ray diffractio
n and energy-dispersive X-ray analysis of equilibrated samples. There
is only one quaternary oxide CaNiSi2O6 with clinopyroxene structure. T
he Gibbs energy of formation of CaNiSi2O6 is measured using a solid st
ate galvanic cell incorporating stabilized zirconia as the solid elect
rolyte in the temperature range of 1000 to 1400 K: Pt, Ni + SiO2 + CaS
iO3 + CaNiSi2O6 \ (Y2O3)ZrO2 \ Ni + NiO, Pt From the electromotive for
ce (emf) of the cell, the Gibbs energy of formation of CaNiSi2O6 from
NiO, SiO2, and CaSiO3 is obtained. To derive the Gibbs energy of forma
tion of the quaternary oxide from component binary oxides, the free en
ergy of formation of CaSiO, is determined separately using a solid sta
te cell based on single crystal CaF2 as the electrolyte: Pt, O-2, CaO
+ CaF2 \ CaF2 \ CaSiO3 + SiO2 + CaF2, O-2, Pt The results can be expre
ssed by the following equations: NiO (r.s) + CaO (r.s) + 2SiO(2) (qz)
--> CaNiSi2O6 (pyr) Delta G degrees = -115,700 + 10.63T (+/-100) J mol
(-1) CaO (r.s) + SiO2 (qz) --> CaSiO3 (wol) Delta G degrees = -90,030
-0.61T (+/-60) J mol(-1).