1983
DOI: 10.1016/0001-6160(83)90219-5
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On the kinetics of structural relaxation in metallic glasses

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Cited by 225 publications
(44 citation statements)
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“…Second, taking the experimental molar heat of structural relaxation Q µ and calculating the number of defects per mole, N µ = ∆cN A , (∆c is the averaged number of defects annealed out during structural relaxation, N A the Avogadro number), one can determine the heat of structural relaxation per defect, Q d = Q µ /N µ . On the other hand, one can calculate the interstitialcy formation enthalpy using Equation (12). Table 1 illustrates a remarkable similarity between the heat of structural relaxation per defect Q d and interstitialcy formation enthalpy H: the difference between these quantities is less than 4%.…”
Section: Rt Xmentioning
confidence: 97%
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“…Second, taking the experimental molar heat of structural relaxation Q µ and calculating the number of defects per mole, N µ = ∆cN A , (∆c is the averaged number of defects annealed out during structural relaxation, N A the Avogadro number), one can determine the heat of structural relaxation per defect, Q d = Q µ /N µ . On the other hand, one can calculate the interstitialcy formation enthalpy using Equation (12). Table 1 illustrates a remarkable similarity between the heat of structural relaxation per defect Q d and interstitialcy formation enthalpy H: the difference between these quantities is less than 4%.…”
Section: Rt Xmentioning
confidence: 97%
“…Since the density is increasing upon structural relaxation of initial MGs below T g , it is widely believed that elementary structural relaxation events take place in the regions of smaller local density, i.e., in the regions containing some excess "free volume" [4,9,12,13]. In spite of the fact that the "free volume" has no clear theoretical definition, as repeatedly mentioned in the literature (e.g., [17,85]), and the application of this concept to the interpretation of experimental data sometimes leads to evident inconsistencies [16,77], the free volume-based notions still remain quite popular [4,11,15,86].…”
Section: Interstitialcies Free Volume and Enthalpy Releasementioning
confidence: 99%
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“…By thermal cycling, the annealing induced relaxation can be separated into reversible and irreversible components and has been interpreted by chemical short range ordering (CSRO) and topological short range ordering (TSRO) respectively [21,22]. The former was explained by the activation energy spectrum, while the latter was explained in terms of free volume theory [21].…”
Section: T T T Tmentioning
confidence: 99%
“…Since volume decreases as a result of structural relaxation, it is often interpreted in terms of decrease in free-volume. [32] However, volume decrease is only a part of the entire array of properties that change as a result of structural relaxation. [33] Whereas the change in volume is quite small, usually of the order of a few tenths of a percent, the heat released by relaxation is a substantial portion of the heat of crystallization.…”
Section: Structural Relaxation In Bulk Metallic Glassesmentioning
confidence: 99%