T. Mathews et Kt. Jacob, PHASE-RELATIONS IN THE SYSTEMS CU-O-R2O3 (R=TM,LU) AND GIBBS ENERGIESOF FORMATION OF CU2R2O5 COMPOUNDS, Journal of materials chemistry, 3(10), 1993, pp. 1025-1029
The phase relations in the systems Cu-O-R2O3 (R=Tm, Lu) have been dete
rmined at 1273 K by X-ray diffraction, optical microscopy and electron
probe microanalysis of samples equilibrated in evacuated quartz ampul
es and in pure oxygen. Only ternary compounds of the type Cu2R2O5 were
found to be stable. The standard Gibbs energies of formation of the c
ompounds have been measured using solid-state galvanic cells of the ty
pe, Pt\Cu2O+CU2R2O5+R2O3 \\ (Y2O3)ZrO2 \\ CuO+Cu2O \ Pt in the tempera
ture range 950-1325 K. The standard Gibbs energy changes associated wi
th the formation of CU2R2O5 compounds from their binary component oxid
es are: 2CuO(s)+Tm2O3(S)-->Cu2TM2O5(S), DELTAG-degrees = (10400-14.0 T
/K) +/- 100 J mol-1 2CuO(s)+Lu2O3(S)-->Cu2Lu2O5(S), DELTAG-degrees = (
10210-14.4 T/K) +/- 100 J mol-1 Since the formation is endothermic, th
e compounds become thermodynamically unstable with respect to componen
t oxides at low temperatures, Cu2TM2O5 below 743 K and Cu2LU2O5 below
709 K. When the chemical potential of oxygen over the CU2R2O5 compound
s is lowered, they decompose according to the reaction, 2Cu2R2O5(S)-->
2R2O3(S) + 2Cu2O(S) + O2(g) The equilibrium oxygen potential correspon
ding to this reaction is obtained from the emf. Oxygen potential diagr
ams for the Cu-O-R2O3 systems at 1273 K are presented.