Polymer Networks: Structure and Mechanical PropertiesA. Chompff, Seymour Newman For several decades, polymer science has sought to rationalize the mechanical and thermodynamic properties of polymer networks largely within the framework of statistical thermodynamics. Much of this effort has been directed toward the rubbery rather than the glassy state. It is generally assumed that networks possess an av erage composition to which average properties may be assigned; from such a continuum view, a powerful analysis of such properties as modulus, swelling, birefringence and thermoelasticity has emerged. In the years following the rise of polymer characterization (the late 40's and early 50's), many scientists began to study ap parent relations between the properties of linear polymer molecules and the networks obtainable therefrom. This search was also stimu lated by the wide range of applications of polymer networks in com mercial elastomers, thermosets and coatings. Frequently, these data were confidently matched with curves obtained from statisti cally describable models of networks of ghost chains, uniformly distributed in space. More recently, it has become apparent that polymer chains in networks are not as ideal as assumed in the formulation of statis tical models, and there has been a shift in emphasis towards the less than ideal, perturbed and possibly inhomogeneous networks which are more frequently encountered in practice. The continuum approach, however, had to be developed before inhomogeneous systems could be described; the present volume, therefore, contains both views. |
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Page 293
... particle providing the rubber remains attached to this particle . Consequently , the degree of swelling in the immediate vicinity of the filler particle will be less than in the bulk of the rubber and there will be a gradient of ...
... particle providing the rubber remains attached to this particle . Consequently , the degree of swelling in the immediate vicinity of the filler particle will be less than in the bulk of the rubber and there will be a gradient of ...
Page 301
... particle sizes about 8μ which is in the range of sizes of the particles introduced in the rubber . On the other hand , the secondary maximum intensity is about a hundred times weaker than the first maximum intensity and as the ...
... particle sizes about 8μ which is in the range of sizes of the particles introduced in the rubber . On the other hand , the secondary maximum intensity is about a hundred times weaker than the first maximum intensity and as the ...
Page 345
... particle- particle association and possibly also particle - polymer breakdown could account for the effect [ 3-5 ] . Later Bueche [ 7,8 ] proposed a molecular model for the Mullins ' Effect based on the assumption that the centers of ...
... particle- particle association and possibly also particle - polymer breakdown could account for the effect [ 3-5 ] . Later Bueche [ 7,8 ] proposed a molecular model for the Mullins ' Effect based on the assumption that the centers of ...
Contents
Chemical and Physical Aspects of the Three Stages | 1 |
On the Thermostatic Behavior of Elastomers | 23 |
Thermoelasticity of Crosslinked Rubber Networks | 47 |
Copyright | |
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angle behavior birefringence branch points calculated chain ends Chem chemical coefficient components composition constant constitutive equation copolymer correlation cross crosslink density crosslinking agent curve deformation degree dependence diluent divinyl dynes/cm² effect elastic elastomer elements epoxy equilibrium experimental Figure filler Flory fracture energy free energy free volume function Galcit Gaussian gel point given glass point highly crosslinked homogeneous increase inhomogeneous integration interaction IPN's light scattering linear macromolecules material matrix measurements mechanical molecular weight molecules monomer natural rubber network chains non-linear obtained orientation parameters particle phase separation Phys plane plastic plotted PMMA poly polymer chains polymer networks Polymer Sci polymeric polystyrene prepolymer properties reaction refractive index rupture sample segments shown solid strain energy Strain Input stress stress-strain structure styrene surface energy swelling swollen Table temperature tensile strength tension theoretical theory tion values viscoelastic zero