The conductivities of solid solutions which contained 10mol% of a rare-earth oxide were measured (table 151) in order to determine the form of the temperature variation. It was found that the Arrhenius plots were broken straight lines, with a number of linear sections which depended upon the nature of the added ion. There was a decrease in the number of linear segments, and a shift of the low-temperature break towards higher temperatures, as the radius and polarizability of the rare-earth ion increased (see entries for ZrO2-Gd2O3, ZrO2-Ho2O3, ZrO2-Nd2O3, ZrO2-Sc2O3, ZrO2-Lu2O3 and ZrO2-Yb2O3).
A.N.Vlasov: Elektrokhimiya, 1989, 25[5], 699-702
Table 151
Ionic Conduction Parameters for ZrO2-10mol%Y2O3
Temperature (K) | ln[o (SK/cm)] | E (kJ/mol) |
1770-1520 | 5.21 | 70 |
1520-1200 | 5.49 | 78 |
1200-1010 | 5.88 | 87 |
1010-750 | 6.55 | 99 |
< 750 | 7.07 | 107 |
Y: ionic radius = 0.0900, polarizability = 0.0015