Solution softening in spinel

The critical resolved shear stress of MgO.nAl sub 2 O sub 3 spinel at a given temperature decreases dramatically, by almost two orders of magnitude, with increasing deviation from stoichiometry, i.e., as n increases from 1-3.5. The CRSS is proportional to exp(-T/T sub 0 ) and to [V sub c ] exp -2 ,...

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Veröffentlicht in:Scripta Materialia 1998-08, Vol.39 (4), p.537-544
Hauptverfasser: Mitchell, T.E., Donlon, W.T., Heuer, A.H.
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Donlon, W.T.
Heuer, A.H.
description The critical resolved shear stress of MgO.nAl sub 2 O sub 3 spinel at a given temperature decreases dramatically, by almost two orders of magnitude, with increasing deviation from stoichiometry, i.e., as n increases from 1-3.5. The CRSS is proportional to exp(-T/T sub 0 ) and to [V sub c ] exp -2 , where T sub 0 is a characteristic temperature and [V sub c ] is the concentration of charge-compensating cation vacancies. Slip on {111} planes is thought to occur between the Kagome cation layers and the adjacent anion layers. Slip on {101} planes is slightly easier (and has a higher T sub 0 ) because the planes are more widely separated. Slip in spinel does not require synchro-shear, unlike slip in the C15 AB sub 2 Laves phase, which has identical metal atom positions to the cation positions in spinel. The temperature dependence of the CRSS is analyzed in terms of a model based on partial dislocations overcoming a steep and high Peierls potential. Parameters for the model can be chosen to explain the observed values of T sub 0 and the CRSS extrapolated to T=0K for both spinel and sapphire. Other models are possible. The dependence of CRSS on [V sub c ] exp -2 can be explained in terms of kink nucleation at cation vacancies.
doi_str_mv 10.1016/S1359-6462(98)00194-8
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The CRSS is proportional to exp(-T/T sub 0 ) and to [V sub c ] exp -2 , where T sub 0 is a characteristic temperature and [V sub c ] is the concentration of charge-compensating cation vacancies. Slip on {111} planes is thought to occur between the Kagome cation layers and the adjacent anion layers. Slip on {101} planes is slightly easier (and has a higher T sub 0 ) because the planes are more widely separated. Slip in spinel does not require synchro-shear, unlike slip in the C15 AB sub 2 Laves phase, which has identical metal atom positions to the cation positions in spinel. The temperature dependence of the CRSS is analyzed in terms of a model based on partial dislocations overcoming a steep and high Peierls potential. Parameters for the model can be chosen to explain the observed values of T sub 0 and the CRSS extrapolated to T=0K for both spinel and sapphire. Other models are possible. The dependence of CRSS on [V sub c ] exp -2 can be explained in terms of kink nucleation at cation vacancies.</abstract><cop>New York, NY</cop><pub>Elsevier Ltd</pub><doi>10.1016/S1359-6462(98)00194-8</doi><tpages>8</tpages></addata></record>
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subjects ALUMINIUM OXIDES
Condensed matter: structure, mechanical and thermal properties
DISLOCATIONS
Exact sciences and technology
Fatigue, brittleness, fracture, and cracks
MAGNESIUM OXIDES
MATERIALS SCIENCE
Mechanical and acoustical properties of condensed matter
Mechanical properties of solids
MICROSTRUCTURE
Physics
SHEAR PROPERTIES
SLIP
STOICHIOMETRY
TEMPERATURE DEPENDENCE
VACANCIES
title Solution softening in spinel
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