The critical role of entropy in glass transition kinetics
arXiv:2501.11857 · doi:10.1007/s11433-025-2707-5
Abstract
Glass transition is a reversible transition that occurs in most amorphous materials. However, the nature of glass transition remains far from being clarified. A key to understand the glass transition is to clarify what determines the glass transition temperature (Tg) and liquid fragility (m). Here the glass transition thermodynamics for 150 different glass-forming systems are studied statistically. It is found that the activation characters in the energy landscape are crucial to precisely portray the glass transition and, in particular, both the activation free energy (G*) and the activation entropy (S*) play critical roles. G* determines Tg, Tg=G*/290+25.5, while S* determines m, m=S*/Rln10+15 with R is gas constant. Based on the Boltzmann definition of entropy, the fragility is an indication of the number of the degeneracy of the evolution paths. This explains why the nano-confined, low-dimension or high-pressured glasses exhibit stronger characteristics, which has been a puzzling phenomenon for a long time.
arXiv comment7 pages, 4 figures
References in corpus (6)
- The relationship between fragility, configurational entropy and the potential energy landscape of glass forming liquids
- Tuning of tetrahedrality in a silicon potential yields a series of monatomic (metal-like) glassformers of very high fragility
- Glass transition and random close packing above three dimensions
- The instantaneous shear modulus in the shoving model
- Relaxation and vibrational properties in metal alloys and other disordered systems
- Exploring canyons in glassy energy landscapes using metadynamics