Abstract
As has been pointed out by A.S. Lodge1) , the constitutive equation for the ideal rubber forms an advantageous starting point for the construction of suitable constitutive equations for polymeric fluids. On the other hand, it is well known that real rubbery materials do not obey the ideal equations derived from the statistical theory. From these facts it appears worth while to start the chapter on the theory of rubber-like liquids with a discussion of the main problems arising in the description of rubber elasticity.
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Janeschitz-Kriegl, H. (1983). Quasi-Molecular Phenomenological Theories. In: Polymer Melt Rheology and Flow Birefringence. Polymers Properties and Applications, vol 6. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-68822-5_2
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DOI: https://doi.org/10.1007/978-3-642-68822-5_2
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