Electrical conductivity and thermopower measurements have been made on Fe3O4-FeCr2O4, Fe3O4-MgCr2O4, and Fe3O4-FeCr2O4-FeAl2O4 spinel sotid solutions at 600 °C to 1400°C and 1 atm. Our analysis of the data indicates that these are n-type small polaron conductors with, as in Fe3O4, electron hopping confined to the octahedral sites. If Cr3+ is not involved in the conduction mechanism (i.e., Fe2+-Fe3+ hopping only) then, with octahedral site hopping, the combined thermopower-electrical conductivity technique enables high-temperature cation distributions to be obtained.

On the Fe3O4-FeCr2O4 join we have found, from measurements of the independent density of states, that hopping is octahedral and involves Fe2+ and Fe3+ only at compositions with 40% or more of Fe3O4, but that Cr3+ becomes involved in the conduction process at very FeCr2O4-rich compositions. We have therefore excluded data on very Crrich compositions, which also exhibit high activation energies, from our estimates of cation distributions.

The thermopower and electrical conductivity data were combined with earlier results on the joins Fe3O4-MgFe2O4, Fe3O4-FeAl2O4, and Fe3O4-MgAl2O4 to estimate cation distributions for compositions within the geologically important system (Mg2+,Fe2+)-(Fe3+,Al3+,Cr3+)2O4. The cation distributions were then combined with activity-composition relations and interphase partitioning data to derive a complete thermodynamic model for the complex system (Mg2+,Fe2+)(Fe3+,Al3+,Cr3+)2O4. The model, which takes explicit account oforder-disorder relations, produces and successfully predicts a wide range of macroscopic thermodynamic measurements that have been made on simple and complex spinels. A computer program to generate cation distributions and activities is available from B. J. Wood.

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