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The statistical mechanics of polymerized material

1967/09/01 by S. F. Edwards · 4 citations
Physics and Astronomy · Chemical Engineering · Computer Science · #Advanced Mathematical Theories and Applications #Rheology and Fluid Dynamics Studies #Data Visualization and Analytics

paper · doi:10.1088/0370-1328/92/1/303

openalex publication_date 1967/09/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/04

Abstract

It is argued that a solid consisting of fully entangled long chain molecules will show elastic properties similar to those of cross linked, i.e. vulcanized material, provided that elastic moduli are studied in periods short compared with creep times. An appropriate formula for the free energy is deduced, and calculated for a model in which each chain is confined to an environment formed by the others. Under deformation this environment changes and the elastic energy can be deduced. If 1 , 2 , 3 are the principal strains, that part of the free energy due to the polymer entanglements is shown to be Δ F = - B κ T ( 1 2 + 2 2 + 3 2 ) L (σ l/m ) 1/2 for small strains, where B is a numerical constant, L is the total length of polymer present, σ the density of polymer, and l, m the effective length and mass of one of the submolecules from which the polymer is made. An expression is also given for the case of a strain of arbitrary size.

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