From owner-biophysics@net.bio.net Mon Feb 16 22:00:00 1998 Path: biosci!agate!logbridge.uoregon.edu!newsfeed.direct.ca!news-peer.sprintlink.net!news.sprintlink.net!Sprint!worldnet.att.net!news.u.washington.edu!fujimoto From: fujimoto@u.washington.edu (Bryant Fujimoto) Newsgroups: bionet.biophysics Subject: Re: Boltzmann's versus thermodynamic entropy Date: 17 Feb 1998 21:32:43 GMT Organization: University of Washington Lines: 24 Distribution: bionet Message-ID: <6ccvlr$3pk$1@nntp3.u.washington.edu> References: <6cbibd$5m0@mserv1.dl.ac.uk> NNTP-Posting-Host: homer18.u.washington.edu X-Trace: nntp3.u.washington.edu 887751163 3892 (None) 140.142.64.1 X-Complaints-To: help@cac.washington.edu NNTP-Posting-User: fujimoto Pentcho Valev writes: >Andras, I do not see any contradiction between my statement and your >explanation, so there is certainly nothing which I don't understand at >that level. Still I find it awkward to accept that, as the system >(rather, only D) expands spontaneously and never returns to the initial >point, it moves from a MORE probable to a LESS probable state. Your >explanation is formally correct but it contradicts my intuition. Your intuition is wrong. You haven't even proved which way the heat will flow. How do you know heat will flow out of the chamber? You haven't accounted for the heat necessary to maintain the temperature as you expand your system. >Unfortunately I am incompetent in statistical mechanics and cannot offer >a more reasonable objection. Still my conclusion remains valid: The >two entropies may coincide but ONLY IF SYSTEMS CAN SPONTANEOUSLY MOVE >FROM A MORE PROBABLE TO A LESS PROBABLE STATE. If your conclusion is valid, then why is it contradicted by every test ever made to compare statisical mechanical and thermodynamic entropies? Bryant .