The self-diffusion of O was measured (using 18O and secondary ion mass spectroscopy) in monocrystals and polycrystals of -Al2O3, doped with Y2O3, at temperatures ranging from 1110 to 1630C. In the case of the monocrystals, 2 mechanisms were involved. These were a bulk diffusion mechanism and a sub-boundary one. Both mechanisms were observed at high temperatures while, at lower temperatures, bulk diffusion predominated. The lattice and sub-boundary diffusion coefficients could be described by:
D (cm2/s) = 67 exp[-590(kJ/mol)/RT]
and
D (cm2/s) = 1017exp[-977(kJ/mol)/RT]
respectively. In the case of the polycrystals, the grain boundary diffusivity could be
described by:
D (cm2/s) = 5 x 1011exp[-835(kJ/mol)/RT]
It was concluded that Y slightly increased O bulk diffusion, and decreased grain boundary diffusion.
M.Le Gall, B.Lesage, N.Brun, A.M.Huntz, M.Miloche, C.Monty: Materials Science Forum, 1993, 126-128, 411-4
Table 8
Bulk Diffusivity of O in Monocrystals of -Al2O3
(doped with 135ppm[mol] of Y2O3)
Temperature (C) | D (cm2/s) |
1110 | 1.6 x 10-17 |
1250 | 8.0 x 10-19 |
1345 | 1.3 x 10-17 |
1370 | 1.6 x 10-17 |
1396 | 2.3 x 10-17 |
1415 | 2.0 x 10-17 |
1460 | 3.0 x 10-17 |
1497 | 1.5 x 10-16 |
1505 | 1.4 x 10-16 |
1550 | 2.8 x 10-15 |
1600 | 1.4 x 10-15 |
1614 | 3.0 x 10-15 |
1630 | 1.4 x 10-14 |