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Flory-Huggins solution theory
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Flory-Huggins solution theory is a mathematical model of the thermodynamics of polymer solutions which takes account of the great dissimilarity in molecular sizes in adapting the usual expression for the entropy of mixing. The result is an equation for the Gibbs free energy change Delta G_m for mixing a polymer with a solvent. Although it makes simplifying assumptions, it generates useful results for interpreting experiments.The thermodynamic equation for the Gibbs free energy change accompanying mixing at constant temperature and (external) pressure is » Delta G_m = Delta H_m - TDelta S_m ,

A change, denoted by Delta, is the value of a variable for a solution or mixture minus the values for the pure components considered separately. The objective is to find explicit formulas for Delta H_m and Delta S_m, the enthalpy and entropy increments associated with the mixing process.
   The result obtained by Flory and Huggins is » Delta G_m = RT[,n_1lnphi_1+ n_2lnphi_2 + n_1phi_2chi_ is the actual volume of a polymer segment.
   This treatment doesn't attempt to calculate the conformational entropy of folding for polymer chains. (See the random coil discussion.) The conformations of even amorphous polymers will change when they go into solution, and most thermoplastic polymers also have lamellar crystalline regions which don't persist in solution as the chains separate. These events are accompanied by additional entropy and energy changes.
   More advanced models exist, such as the Flory-Krigbaum theory.

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