Abstract
The thermal properties of a model liquid are expressed in terms of the properties of the glasses that it samples. Each glass is modeled as an Einstein solid with enthalpy H0 at absolute zero and an Einstein temperature that decreases linearly with H0. The number of glasses with enthalpy H0 is represented by a Gaussian distribution. The range over which the liquid exists is bounded below by a Kauzmann temperature, where it has the same entropy as an individual glass, and bounded above by a heat capacity divergence.
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
