A simple connection between the melting temperature and the glass temperature in a kinetic theory of the glass transition

1992 ◽  
Vol 4 (32) ◽  
pp. L429-L431 ◽  
Author(s):  
A Hunt
1981 ◽  
Vol 8 ◽  
Author(s):  
Mats Hillert

ABSTRACTThe kinetic theory of the glass transition is examined. Some modifications are suggested in order to overcome some shortcomings. As a result, a thermodynamic description of the glass transition is obtained. It is demonstrated that the glass transition represents the beginning of a very gradual process of melting in the amorphous state.


2016 ◽  
Vol 186 (1) ◽  
pp. 47-73 ◽  
Author(s):  
Timur V. Tropin ◽  
Juern W.P. Schmelzer ◽  
Viktor L. Aksenov

1998 ◽  
Vol 554 ◽  
Author(s):  
G. Wilde ◽  
J. H. Perepezko

AbstractThe enthalpy, entropy, specific heat, specific volume and the equilibrium shear viscosity of the deeply undercooled melt of the bulk glass forming alloy Pd40Ni40P20 have been determined as functions of temperature. The concept of limiting fictive temperature was applied to the entire set of measurements in order to allow for a valid comparison of the data based upon the respective equilibrium values. The comparison of the equilibrium properties shows that a proposed hierarchy of stability limits does not apply for this alloy. The results also indicate that the glass temperature as defined by the limiting fictive temperature does not depend on the property under observation.


1977 ◽  
Vol 55 (13) ◽  
pp. 2517-2522 ◽  
Author(s):  
D. Ceccaldi

A general kinetic theory is used to explain the shapes of photoionized sample luminescence curves perturbed by thermal jumps (Δ ∼ 1 K, rise time ∼ 1 s). The samples studied are photoactivated organic vitreous solutions of TMPD/MCH 10−3 M and TMPD/3-MP 10−3 M. The experiments are performed within a temperature range (63–91 K) which includes the glass transition temperature Tg. It is shown that there is a slow diffusion of the trapped electrons towards the cation and competition between thermal detrapping and tunneling. The tunneling/thermal detrapping ratio Y is not time dependent during an isothermal luminescence and is only slowly temperature dependent if T ≤ Ty. Ty is very close to Tg. For T > Ty, Y decreases rapidly with T. The activation energy for thermal detrapping shows a maximum when the temperature reaches [Formula: see text] The glass transition temperature Tg may therefore be defined empirically as:[Formula: see text]Finally we obtain a glassy matrix relaxation time, τ, which decreases with T.


2016 ◽  
Vol 59 (1) ◽  
pp. 42-66 ◽  
Author(s):  
T V Tropin ◽  
J W Schmelzer ◽  
V L Aksenov

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