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.
Full Text 
Sign-in/Register to access full text options
Sign-in/Register to access full text options 
Published version (
Free)
Free) 
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 call
