Isothermal sections of the phase diagrams for the systems
Ln–Pd–O (with
Ln=Tb or Er) have been established by equilibration of samples at
T=1223K, and phase identification after quenching by optical and scanning electron microscopy (OM, SEM), energy dispersive spectroscopy (EDS), and X-ray powder diffraction (XRPD). Two oxide phases were stable along the binary Tb–O:
Tb2O3+x, a phase of variable composition, and
Tb7O12 at
T=1223K. The oxide PdO was not stable at this temperature. Only one ternary oxide
Tb2Pd2O5 was identified in the Tb–Pd–O system. No ternary compound was found in the system Er–Pd–O at
T=1223K. However, the compound
Er2Pd2O5 could be synthesized at
T=1075K by the hydrothermal route. In both systems, the alloys and inter-metallic compounds were all found to be in equilibrium with the lanthanide sesquioxide
Ln2O3 (where
Ln is either Tb or Er). Two solid-state cells, each incorporating a buffer electrode, were designed to measure the Gibbs energy of formation of the ternary oxides, using yttria-stabilized zirconia as the solid electrolyte and pure oxygen gas as the reference electrode. Electromotive force measurements were conducted in the temperature range (900–1275)K for Tb–Pd–O system, and at temperatures from (900–1075)K for the system Er–Pd–O. The standard Gibbs energy of
ΔfGm, formation of the inter-oxide compounds from their component binary oxides
Ln2O3 and PdO
ΔfGm, are represented by equations linear in temperature. Isothermal chemical potential diagrams for the systems
Ln–Pd–O (with
Ln=Tb or Er) are developed based on the thermodynamic information.