PostprintThis is the accepted version of a paper published in Journal of Chemical Physics. This paper has been peer-reviewed but does not include the final publisher proof-corrections or journal pagination.
Citation for the original published paper (version of record):Andersson, O., Johari, G P. (2016) Sub-Tg features of glasses formed by cooling glycerol under pressure -Additional incompatibility of vibrational with configurational states in the depressurized, high density glass.
Journal of Chemical Physics
AbstractThe vibrational state of a glass is naturally incompatible with its configurational state, which makes the glass structurally unstable. When a glass is kept at constant temperature, both the vibrational and configurational states of a glass change with time until (equilibrium) liquid state is reached, and the two states become compatible. The process, known as structural relaxation, occurs at a progressively higher rate during heating and the properties of a glass change accordingly. We add to this incompatibility by depressurizing a glass that had been formed by cooling a liquid under a high pressure, p, and then investigate the effects of the added incompatibility by studying thermal conductivity, , and the heat capacity per unit volume C p of the depressurized glass. We use glycerol for the purpose, and study first the changes in the features of , and of C p during glass formation on cooling under a set of different p. We then partially depressurize the glass and study the effect of the p-induced instability on the features of and C p as the glass is isobarically heated to the liquid state. At a given low p, the glass configuration that was formed by cooling at high-p had a higher than the glass configuration that was formed by cooling at a low p. The difference is more when the glass is formed at a higher p and/or is depressurized to a lower p. On heating at a low p, its decreases before its glass-liquid transition range is reached. The effect is the opposite of the increase in observed on heating a glass at the same p under which it was formed. It is caused by thermallyassisted loss of the added incompatibility of configurational and vibrational states of a high-p formed glass kept at low p. If a glass formed under a low-p is pressurized and then heated under high p, it would show the opposite effect, i.e., its would first increase to its high p value before its glass-to-liquid transition range. a joharig@mcmaster.ca 2