The conductivity was measured as a function of composition, temperature and frequency. The degree of enhancement of the conductivity was generally of the order of 50-fold, although an enhancement which amounted to 3 orders of magnitude was sometimes found (table 224). The degree of enhancement was markedly dependent upon the size of the dispersed particles. For a given particle size, the various additions gave different degrees of enhancement. It was concluded that the enhancement arose from bulk, rather than grain-boundary or surface, conduction effects. It was suggested that the dispersed particles led to the generation of an excess of lattice defects, such as Ag+ ion vacancies, in the AgI-Al2O3 system. The excess defects were then expected to enhance the conductivity.
K.Shahi, J.B.Wagner: Journal of Solid State Chemistry, 1982, 42[2], 107-19
Table 224
Ionic Conduction Parameters for AgI-AgBr
AgBr (mol%) | Temperature (C) | σo (S/cm) | Q (eV) |
1 | 25-110 | 2.83 x 102 | 0.52 |
2 | 25-110 | 9.29 x 101 | 0.46 |
4 | 25-100 | 2.37 x 101 | 0.40 |
10 | 25-85 | 4.29 x 10-1 | 0.26 |
15 | 25-80 | 1.46 x 100 | 0.25 |
20 | 25-80 | 1.70 x 100 | 0.22 |