2019
DOI: 10.1016/j.jallcom.2019.03.106
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Melt viscosity of nanocrystalline alloys in the model of free volume

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Cited by 11 publications
(12 citation statements)
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“…Since after cooling the viscosity of the melts does not recover to its initial value, it can be concluded that the melt underwent irreversible changes. The viscosity of Fe 73.5 Cu 1 M 3 Si 13.5 B 9 melts with various inhibitors correlates well with the free volume [36]. The Nb melt has the largest free volume, while the Mo melt has the smallest.…”
Section: Multicomponent Meltsmentioning
confidence: 83%
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“…Since after cooling the viscosity of the melts does not recover to its initial value, it can be concluded that the melt underwent irreversible changes. The viscosity of Fe 73.5 Cu 1 M 3 Si 13.5 B 9 melts with various inhibitors correlates well with the free volume [36]. The Nb melt has the largest free volume, while the Mo melt has the smallest.…”
Section: Multicomponent Meltsmentioning
confidence: 83%
“…The reason for the oscillations can be a transition from a non-equilibrium melt structure inherited from the initial crystalline phases to an equilibrium state, or random oscillations associated with the periodic appearance and destruction of cluster structures, or an intense structural transformation of the melt [35]. Figure 4 shows the kinematic viscosity in logarithmic scale and absolute temperature in the inverse scale for Fe 73.5 Cu 1 M 3 Si 13.5 B 9 melts with different inhibitors M = Nb, Mo, V, Cr at the stage of heating (a) and cooling (b) [36]. At the heating stage, the temperature dependences of melts with Nb, Mo, and V have two linear sections, the slope of which changes at the critical temperature T k = 1770 K. In a melt with Nb, the activation energy increases upon going to the high-temperature region.…”
Section: Multicomponent Meltsmentioning
confidence: 99%
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