Abstract
The Flory-Huggins lattice treatment has been the cornerstone for many years for understanding the solution thermodynamics of flexible polymers. The effect of chain stiffness was investigated by Flory, again using a lattice approach,1,2 where the stability of both ordered and disordered phases was considered. The phase equilibria for a rigid rod-diluent system, plotted as the volume fraction vi, are shown in Figure 1 for a rod of 150 axial ratio, where χ is the van Laar polymer-solvent heat of mixing parameter. Alternatively, χ may be looked upon as proportional to the excess free energy of mixing.
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References
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Wee, E.L., Miller, W.G. (1978). Lattice Model Treatments of the Formation of Ordered Phases in Stiff Chain Polymer-Diluent Systems. In: Johnson, J.F., Porter, R.S. (eds) Liquid Crystals and Ordered Fluids. Springer, Boston, MA. https://doi.org/10.1007/978-1-4615-8888-7_26
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DOI: https://doi.org/10.1007/978-1-4615-8888-7_26
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