Thermochimica Acta 484 (2009) 70–76
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Thermochimica Acta
journal homepage: www.elsevier.com/locate/tca
On the glass-crystal transformation kinetics by using differential scanning
calorimetry under non-isothermal regime
Application to the crystallization of the Ag
0.16
As
0.46
Se
0.38
semiconductor glass
J.L. Cárdenas-Leal, J. Vázquez
∗
, D. García-G. Barreda, P.L. López-Alemany, P. Villares, R. Jiménez-Garay
Departamento de Física de la Materia Condensada, Facultad de Ciencias, Universidad de Cádiz, Apartado 40, 11510 Puerto Real (Cádiz), Spain
article info
Article history:
Received 24 March 2008
Received in revised form 5 November 2008
Accepted 30 November 2008
Available online 9 December 2008
PACS:
61.40
64.40.Qb
64.70.Kb
64.70.Pf
Keywords:
Amorphous materials
Glass-crystal transformation
Impingement effect
Differential scanning calorimetry
Reheating treatment
Thermal analysis
abstract
A procedure has been developed to obtain an evolution equation with the temperature for the actual
transformed volume fraction under non-isothermal regime, to calculate the kinetic parameters and to
analyze the glass-crystal transformation mechanisms in solid systems where a large number of nuclei
already exists and no other new nuclei are formed during the thermal treatment. In this case, it is assumed
that the nuclei only grow, “site saturation”, during the thermal process. Once an extended volume of
transformed material has been defined and spatially random transformed regions have been assumed, a
general expression of the extended volume fraction has been obtained as a function of the temperature.
Considering the mutual interference of regions which grow from separate nuclei (impingement effect)
and from the quoted expression, the actual transformed volume fraction has been deduced. The kinetic
parameters have been obtained, by assuming that the reaction rate constant is a time function through its
Arrhenian temperature dependence. The developed theoretical method has been applied to the crystal-
lization kinetics of the Ag
0.16
As
0.46
Se
0.38
glassy alloy as-quenched and previously reheated. In accordance
with the corresponding results, it is possible to establish that in the considered alloy the nuclei were dom-
inant before the thermal treatment, and because of it the reheating does not change in a considerable way
the number of the pre-existing nuclei in the material, which is a case of “site saturation”. The comparison
of the quoted results with the values obtained by means of Matusita method confirms the reliability of the
theoretical method developed (TMD). Moreover, the obtained values for the kinetic parameters coincide
in a satisfactory way with the results calculated by means of the Austin–Rickett (AR) equation under non-
isothermal regime. Besides, the experimental curve of the transformed fraction shows a better agreement
with the theoretical curves of the developed method and of the Austin–Rickett model than with the cor-
responding curve of the Avrami model. Accordingly, it seems appropriate to choose the Austin–Rickett
equation in order to describe the crystallization mechanism of the above-mentioned glassy alloy.
© 2008 Elsevier B.V. All rights reserved.
1. Introduction
Traditionally, solid-state physics has meant crystal physics.
Solidity and crystallinity have been considered as synonymous in
texts on condensed matter. However, at present one of the most
active fields of solid-state research is the study of solids that are
not crystals, solids in which the arrangement of the atoms lacks the
slightest vestige of long-range order. Solid-state phase transforma-
tions play an important role in the production of many materials.
Therefore, the last decades have seen the strong impulse that
research community has given at the study of a general descrip-
tion of the kinetics of phase transformations [1] and accordingly,
during the last 60 years the theoretical and practical interest in the
∗
Corresponding author.
E-mail address: jose.vazquez@uca.es (J. Vázquez).
application of calorimetric analysis techniques to the study of the
quoted transformations has notably increased [2–4]. Thus, the for-
mal theory of nucleation and crystal growth has been developed
during the last half century with the notable work performed by
Christian [5] and a relatively recent review published by Kelton
[6]. The calorimetric analysis techniques are quick and need small
quantities of glass samples to obtain the kinetic parameters of a
transformation. There are two thermal analysis regimes: isothermal
and non-isothermal. The first one is in most cases more accu-
rate and the data can be interpreted by the Johnson–Mehl–Avrami
(JMA) equation [7–10], however, the non-isothermal thermoana-
lytical methods have several advantages. The rapidity with which
non-isothermal experiments can be performed makes this type of
experiments more attractive. Moreover, the industrial processes
often depend on the kinetic behaviour of systems undergoing
phase transformations under non-isothermal conditions. Accord-
ingly, the use of non-isothermal techniques to study solid-state
0040-6031/$ – see front matter © 2008 Elsevier B.V. All rights reserved.
doi:10.1016/j.tca.2008.11.014