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The Role of Rheology in Polymer Extrusion - Polydynamics, Inc.

The Role of Rheology in Polymer Extrusion - Polydynamics, Inc.

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<strong>The</strong> usefulness <strong>of</strong> this rule, which holds for most polymers, is that while steady measurements <strong>of</strong><br />

shear viscosity are virtually impossible above 5 s –1 with rotational <strong>in</strong>struments, the dynamic<br />

measurements can easily be carried out up to 500 rad/s (corresponds to = 500 s –1 ) or even<br />

higher. Thus, the full range <strong>of</strong> viscosity needed <strong>in</strong> extrusion can be covered.<br />

Some typical results <strong>in</strong>volv<strong>in</strong>g narrow and broad molecular-weight-distribution samples<br />

are shown <strong>in</strong> Figure 1.9. <strong>The</strong> relative behavior <strong>of</strong> G versus can be used to identify whether a<br />

sample is <strong>of</strong> narrow or broad molecular weight distribution [6]. In fact, from the "crossover<br />

po<strong>in</strong>t" where G = G, it is possible to get a surpris<strong>in</strong>gly good estimate <strong>of</strong> the polydispersity<br />

M w /M n for PP [10].<br />

1.5 Constitutive Equations<br />

<strong>The</strong>se are relations between stresses and stra<strong>in</strong>s (deformations). In its simplest form, the<br />

Newtonian equation is<br />

where is viscosity and = du/dy, the shear rate.<br />

fluid<br />

For a shear th<strong>in</strong>n<strong>in</strong>g material <strong>of</strong> the power-law type, we have<br />

where m is consistency and n the power-law exponent.<br />

= <br />

(1.31)<br />

n-1<br />

n<br />

= = m = m <br />

(1.32)<br />

However, the above expressions, when <strong>in</strong>serted <strong>in</strong>to the equation <strong>of</strong> conservation <strong>of</strong><br />

momentum, cannot predict viscoelastic effects such as normal stresses, stress relaxation or<br />

extrudate swell. <strong>The</strong> simplest way to develop viscoelastic constitutive equations is to comb<strong>in</strong>e a<br />

model for an elastic solid<br />

with that for a Newtonian fluid<br />

= G <br />

(1.33)<br />

solid<br />

= <br />

flui d<br />

(1.34)<br />

By differentiat<strong>in</strong>g Equation 1.33 and add<strong>in</strong>g the two stra<strong>in</strong> rates, we get<br />

or<br />

<br />

+ = <br />

G <br />

(1.35)<br />

15

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