Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.2 9/18/84; site psivax.UUCP Path: utzoo!linus!philabs!cmcl2!seismo!hao!hplabs!sdcrdcf!psivax!friesen From: friesen@psivax.UUCP (Stanley Friesen) Newsgroups: net.origins Subject: Re: Now more than ever. PART I Message-ID: <477@psivax.UUCP> Date: Fri, 31-May-85 16:01:59 EDT Article-I.D.: psivax.477 Posted: Fri May 31 16:01:59 1985 Date-Received: Sun, 2-Jun-85 20:39:22 EDT References: <297@cmu-cs-edu1.ARPA> <1556@dciem.UUCP> <884@mhuxt.UUCP> <1200@cbosgd.UUCP> Reply-To: friesen@psivax.UUCP (Stanley Friesen) Distribution: net Organization: Pacesetter Systems Inc., Sylmar, CA Lines: 65 Keywords: entropy, evolution In article <1200@cbosgd.UUCP> rlp@cbosgd.UUCP (Bob Platt) writes: >Summary:applying thermodynamics to evolution > >> from Jeff Sonntag: >> >> ...the second law can be >> applied to evolution only insofar as evolution can be described in terms of >> heat concentration and temperature distributions *or* if entropy can be >> defined somehow in terms which are more descriptive of biological systems. > > This has been attempted, although exactly how succesfully I can't >say, as the mathematics are very complicated and beyond me. My source >is "Structural Stability and Morphogenesis" by Rene Thom (Benjamin/Cummings >1975). I won't reproduce the specific mathematical details here, but the >following quotes give the flavor of Thom's approach: > >"If two systems S1 and S2, with total energy c, are thermodynamically > coupled, the equilibrium regime will occur at the value of t for which >the total entropy S1(c-t) + S2(t) is maximum. If there is only one >sufficiently sharp maximum, the joint system will evolve toward this state >and stay there, neglecting fluctuations. > "The importance of thermodynamical coupling comes from the fact >that, if two dynamical systems over two contiguous open sets U1 and U2 >are put into spatial contact, we can suppose (without any special >hypothesis concerning the nature of the interaction) that the two >systems are thermodynamically coupled." >--- >In the context of evolution, the "two systems" may be interacting >species, such as wasps and orchids: > > "We must not forget that the essential object of study in >biology is not the isolated individual but the continuous form in >space-time joining parents to descendants; more precisely, when two >or more species having some functional interaction between each other, >such as predation or being an auxiliary in the fertilization process, >it is necessary to consider the total figure in space-time, the union >of all forms associated with each species. >--- But this still does not address the other aspect of Jeff Sontag's objection, that is justifying treating a species as a thermodynamic system. Even the quotes only specify *how* one would treat a species as a thermodynamic system, not the reasons why doing so might be permissible. In short Dr Thom is here making a conceptual leap without adequate reasons(at least as far as the quoted excerpts are concerned). The problem with the treatment is that living things are *not* particles on the same sense as atoms in a gas(a typical thermodynamic system). One theoretically important difference is that particles of the same type in the physisist's sense are *indistinguishible* while conspecific organisms are fully distinguishable(that is they are not interchangeable without changing the state of the system). >Thom's ideas are highly speculative, and has been criticized (rightly >or wrongly) for couching his speculations in highly abstract terms >understandable only to highly trained mathematicians. Nevertheless, >he has presented a theory that specifies biological measures of entropy >and information, makes predictions, and is falsifiable. > And in my opinion also for inadequate justification of a major conceptual leap. -- Sarima (Stanley Friesen) {trwrb|allegra|cbosgd|hplabs|ihnp4|aero!uscvax!akgua}!sdcrdcf!psivax!friesen or {ttdica|quad1|bellcore|scgvaxd}!psivax!friesen