Application of the ramp test from a closed cavity rheometer to obtain the steady-state shear viscosity η(γ̇)

Author:

Ellwanger Felix1,Georgantopoulos Christos K.2,Karbstein Heike P.1,Wilhelm Manfred3,Azad Emin M.14

Affiliation:

1. Karlsruhe Institute of Technology (KIT), Institute of Process Engineering in Life Sciences, Chair of Food Process Engineering (LVT) , Gotthard-Franz-Straße 3, 76131 Karlsruhe , Germany

2. VAT Vakuumventile AG, Material and Manufacturing Technology, Core Technology , Seelistrasse 1, 9469 Haag , Switzerland

3. Karlsruhe Institute of Technology (KIT), Institute of Chemical Technology and Polymer Chemistry (ITCP) , Engesserstraße 18, 76131 Karlsruhe , Germany

4. nexnoa GmbH , Aachener Straße 1042, 50858 Köln , Germany

Abstract

Abstract The steady-state shear viscosity η ( γ ̇ ) \eta (\dot{\gamma }) is required in controlling processing parameters for the extrusion processing of polymer melts. A new method, the so-called ramp test, is investigated in this study to obtain the steady-state shear viscosity with a closed cavity rheometer (CCR). To verify the method and the accuracy of the CCR data, three commercial polyolefin polymers, a low-density polyethylene (LDPE), a linear low-density polyethylene (LLDPE), and a polybutadiene (PBD), were used as model systems. Measurements of the magnitude of the complex viscosity η ( ω ) | {\eta }^{\ast }(\omega )| were compared with the steady-state shear viscosity data obtained by capillary rheometer and CCR. Further, time–temperature superposition master curves of the magnitude of the complex viscosity and steady-state shear viscosity obtained by CCR were developed for LLDPE and PBD. The influence of the cavity sealing on the instrument’s accuracy to obtain the steady-state shear viscosity was investigated using the finite element method simulations. Thus, it was shown that the ramp test performed by CCR is a practical method to determine reliable and reproducible data of the steady-state shear viscosity within a wide range of temperatures (T = 50–180°C) for low and high viscous materials ( η ( ω ) | {\eta }^{\ast }(\omega )| = 1.6–480 kPa s, M w = 144–375 kg mol−1).

Publisher

Walter de Gruyter GmbH

Subject

Condensed Matter Physics,General Materials Science

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