ABSTRACT
The behavior of polymers in the solid state results from two forms of organization adopted by the macromolecular chains of glass and crystal. In a glass, the macromolecular chains are by essence at the amorphous state and produce entanglements which participate in the visco-elasticity of the mass material. Reversely, the chains characterized by a regular and symmetrical conformational structure or bearing groups capable of strong molecular interactions of polymers are likely to produce crystalline zones. After presenting the various types of oriented polymers, this article also deals with the incompatibility of polymers between themselves and the difficulty mixing them.
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INTRODUCTION
In the
[AM 3 037]
article, the different types of structures that govern the
geometry of the isolated macromolecule were described: assembly of
atoms and monomer units, tacticity and conformational architectures.
A close relationship exists between this structural level and the
mechanical and thermo-mechanical properties of the final material.
However, many of these properties can only be accounted for through
intermediate structural scales involving the assembly of a more or
less large number of macromolecular chains.
The behavior of polymers in the solid state – as opposed to the
rubbery or viscous state – results from the two forms of organization
that macromolecular chains can adopt, namely those of crystal and
glass. In crystals, polymer chains are organized in a three-dimensional
order, whereas in glass, macromolecular chains are essentially amorphous.
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Morphological structure of polymers