The glass transition width and its dependence on fragility, nonexponentiality and nonlinearity

Abstract

This paper presents a comprehensive and critical analysis of the glass transition width Image ID:d5ma01473e-t3.gif or the reduced width Image ID:d5ma01473e-t4.gif observed in simulated differential scanning calorimetry (DSC) heating and cooling scans. The study employs the Tool-Narayanaswamy-Moynihan model (TNM) for 24 diverse materials, encompassing inorganic glasses, organic polymers and molecular glassy systems. The analysis reveals an important novel finding. The width (or the reduced width) of the glass transition cooling scan is shown to be inversely proportional to the activation energy (h*/R), or fragility index (m), as well as the sum the non-exponentiality β and nonlinearity x parameters, following the relationship: [(h*/R) × (β + x)]−1 or [m × (β + x)]−1. With precise determinations of Tg and Image ID:d5ma01473e-t5.gif, the estimated sum of (β + x) achieves an accuracy comparable to Hutchinson's established peak shift method.

Graphical abstract: The glass transition width and its dependence on fragility, nonexponentiality and nonlinearity

Supplementary files

Article information

Article type
Paper
Submitted
16 Dec 2025
Accepted
14 Mar 2026
First published
17 Mar 2026
This article is Open Access
Creative Commons BY-NC license

Mater. Adv., 2026, Advance Article

The glass transition width and its dependence on fragility, nonexponentiality and nonlinearity

J. Málek, Mater. Adv., 2026, Advance Article , DOI: 10.1039/D5MA01473E

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