Temperature dependence of the plastic flow stress of covalent crystals
A model is presented to explain the steep temperature dependence of the plastic flow stress τ c (T), of highly covalent crystals of α-Al 2 O 3 , Si and GaAs. The model assumes high and steep Peierls potentials: V p (x) = Px 2 + Qx n (n > 2) for x < a/2, a being the period. The kink pair format...
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Veröffentlicht in: | Philosophical magazine. A, Physics of condensed matter. Defects and mechanical properties Physics of condensed matter. Defects and mechanical properties, 1995-02, Vol.71 (2), p.389-397 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | A model is presented to explain the steep temperature dependence of the plastic flow stress τ
c
(T), of highly covalent crystals of α-Al
2
O
3
, Si and GaAs. The model assumes high and steep Peierls potentials: V
p
(x) = Px
2
+ Qx
n
(n > 2) for x < a/2, a being the period. The kink pair formation energy ΔH(τ) is calculated from the elastic interaction energy of a trapezoidal kink pair. The calculation predicts narrow and abrupt kink pairs. The activation energy ΔH(τ) obtained describes the experimental relation log τ
c
= A - BT with constants A and B. The results suggest that the kink pair formation is the rate controlling process of dislocation motion in covalent crystals. |
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ISSN: | 0141-8610 1460-6992 |
DOI: | 10.1080/01418619508244363 |