HANSER Hanser Publishers, Munich • Hanser Gardner Publications ...
HANSER Hanser Publishers, Munich • Hanser Gardner Publications ...
HANSER Hanser Publishers, Munich • Hanser Gardner Publications ...
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1 Formulas of Rheology<br />
One of the most important steps in processing polymers is melting the resin, which is<br />
initially in the solid state, and forcing the melt through a die of a given shape. During this<br />
operation, the melt, whose structure plays a key role in determining the quality of the<br />
product to be manufactured, undergoes different flow and deformation processes.<br />
The plastics engineer has therefore to deal with the melt rheology, which describes the flow<br />
behavior and deformation of the melt. The theory of elasticity and hydromechanics can<br />
be considered the frontier field of rheology, because the former describes the behavior of<br />
ideal elastic solids, whereas the latter is concerned with the behavior of ideal viscous fluids.<br />
Ideal elastic solids deform according to Hooke's Law and ideal viscous fluids obey the<br />
laws of Newtonian flow. The latter are also denoted as Newtonian fluids. Plastic melts<br />
exhibit both viscous and elastic properties.<br />
Thus, the design of machines and dies for polymer processing requires quantitative<br />
description of the properties related to polymer melt flow. Starting from the relationships<br />
for Hookean solids, formulas describing viscous shear flow of the melt are treated first,<br />
as far as they are of practical use in designing polymer machinery. This is followed by a<br />
summary of expressions for steady and time-dependent viscoelastic behavior of melts.<br />
1.1 Ideal Solids<br />
The behavior of a polymer subjected to shear or tension can be described by comparing<br />
its reaction to external force with that of an ideal elastic solid under load. To characterize<br />
ideal solids, first of all it is necessary to define certain quantities as follows [I]:<br />
The axial force Fn in Figure 1.1 causes an elongation A/ of the sample of diameter dQ and<br />
length I0 that is fixed at one end. Following equations apply for this case:<br />
Engineering strain:<br />
Hencky strain:<br />
Tensile stress:<br />
(Li)<br />
(1.2)<br />
(1.3)