Free energy and entropy are examined in detail from the standpoint of
classical thermodynamics. The approach is logically based on the fact that
thermodynamic work is mediated by thermal energy through the tendency for
nonthermal energy to convert spontaneously into thermal energy and for thermal
energy to distribute spontaneously and uniformly within the accessible space.
The fact that free energy is a Second-Law, expendable energy that makes it
possible for thermodynamic work to be done at finite rates is emphasized.
Entropy, as originally defined, is pointed out to be the capacity factor for
thermal energy that is hidden with respect to temperature; it serves to
evaluate the practical quality of thermal energy and to account for changes in
the amounts of latent thermal energies in systems maintained at constant
temperature. A major objective was to clarify the means by which free energy is
transferred and conserved in sequences of biological reactions coupled by
freely diffusible intermediates. In achieving this objective it was found
necessary to distinguish between a 'characteristic free energy' possessed by
all First-Law energies in amounts equivalent to the amounts of the energies
themselves and a 'free energy of concentration' that is intrinsically
mechanical and relatively elusive in that it can appear to be free of First-Law
energy. The findings in this regard serve to clarify the fact that the transfer
of chemical potential energy from one repository to another along sequences of
biological reactions of the above sort occurs through transfer of the First-Law
energy as thermal energy and transfer of the Second-Law energy as free energy
of concentration.Comment: 18-page PDF; major correction in APPENDIX; minor corrections
elsewher