Abstract
We consider the relationship between the Flory-Huggins theory of polymer solutions and self-consistent field theory (SCFT). We show that for uniform solutions, the external field in SCFT is related to the excess chemical potential of a polymer chain and that this is approximated by multiplying the number of segments in the chain by the excess chemical potential of a single segment in a fluid of segments. If the excess chemical potential of the segment is taken to be that of a lattice gas in the Bragg-Williams approximation, one regains the Flory-Huggins expression for the Helmholtz energy. In this approach the Flory-Huggins term commonly ascribed to the entropy of mixing of the solvent, arises directly from the chosen form of the segment excess chemical potential. As for SCFT, a result of this work is the clarification of the nature of the mean-field potential and whether solvent entropic effects have or have not already been taken into account. Copyright © EPLA, 2007.
Original language | English |
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Article number | 26004 |
Journal | EPL |
Volume | 78 |
Issue number | 2 |
DOIs | |
Publication status | Published - 1 Apr 2007 |