TY - JOUR
T1 - The glass transition
T2 - An assessment of current thinking
AU - Angell, C. A.
N1 - Funding Information:
The writer acknowledgessu pporot f this work by the NationalS cienceF oundatiounn derS ohd StateC hemxstry Grant No. DMR 8304887a, ndh elpful& scussxonws athJ . Jackle, L.M. Torell, and S. Yip
PY - 1988/9
Y1 - 1988/9
N2 - Some of the reasons for the current interest in the phenomenology of vitrification are reviewed and progress due to, as well as limitations of, mode coupling theories (MCT) for viscosity divergence are examined. Liquids which fit the MCT predictions best are also those with the most imminent Kauzmann entropy crises near Tg. Mode coupling predictions break down far above Tg at the point, Tx, where Goldstein long ago argued that activated processes controlled by the (3N + 1)-dimensional potential energy surface for the N-particle system should become dominant. Examining behavior in the energy topology-controlled regime, we note that ergodicity-breaking is not simply a consequence of viscosity divergence. In the liquids best fitting MCT, which are at the fragile extreme of liquid behavior, shear and structural relaxation processes slowly decouple below Tx, leading to breakdown of the Adam-Gibbs equation for viscosity. The latter in its original, and derived Vogel-Fulcher, forms remains valid for enthalpy (and presumably volume) relaxation processes. The distinction between strong and fragile behavior in liquids is related to the density of configurational states (minima) characterizing the potential energy surface.
AB - Some of the reasons for the current interest in the phenomenology of vitrification are reviewed and progress due to, as well as limitations of, mode coupling theories (MCT) for viscosity divergence are examined. Liquids which fit the MCT predictions best are also those with the most imminent Kauzmann entropy crises near Tg. Mode coupling predictions break down far above Tg at the point, Tx, where Goldstein long ago argued that activated processes controlled by the (3N + 1)-dimensional potential energy surface for the N-particle system should become dominant. Examining behavior in the energy topology-controlled regime, we note that ergodicity-breaking is not simply a consequence of viscosity divergence. In the liquids best fitting MCT, which are at the fragile extreme of liquid behavior, shear and structural relaxation processes slowly decouple below Tx, leading to breakdown of the Adam-Gibbs equation for viscosity. The latter in its original, and derived Vogel-Fulcher, forms remains valid for enthalpy (and presumably volume) relaxation processes. The distinction between strong and fragile behavior in liquids is related to the density of configurational states (minima) characterizing the potential energy surface.
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U2 - 10.1016/0920-5632(88)90016-3
DO - 10.1016/0920-5632(88)90016-3
M3 - Article
AN - SCOPUS:0011398854
SN - 0920-5632
VL - 5
SP - 69
EP - 80
JO - Nuclear Physics B (Proceedings Supplements)
JF - Nuclear Physics B (Proceedings Supplements)
IS - 1
ER -