Abstract
The first strong-coupling contribution to the canonical entropy of a classical gas is analyzed in the simple case of a Gaussian potential. In agreement with the results by Prigogine et al., it is shown that two different kinds of contributions appear and that only one of them can be identified with the thermodynamical entropy.
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.
