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On the “viscosity overshoot” during the uniaxial extension of a low density polyethylene
Authors:Teodor I Burghelea  Zdeněk Starý  Helmut Münstedt
Institution:1. Université de Nantes, Nantes Atlantique Universités, CNRS, Laboratoire de Thermocinétique de Nantes, UMR 6607, La Chantrerie, Rue Christian Pauc, B.P. 50609, F-44306 Nantes Cedex 3, France;2. Institute of Polymer Materials, Friedrich-Alexander-University, Martensstrasse 7, D-91058 Erlangen, Germany;1. Scitech Associates, LLC, 232 Woodland Drive, State College, PA 16803, USA;2. Department of Physics, 104 Davey Laboratory, The Pennsylvania State University, University Park, PA 16802, USA;3. Facultés Universitaires Notre-Dame de la Paix, Rue de Bruxelles 61, Namur 5000, Belgium;4. Department of Physics, University of Ulsan, Ulsan 680-749, Republic of Korea
Abstract:An experimental investigation of the viscosity overshoot phenomenon observed during uniaxial extension of a low density polyethylene is presented. For this purpose, traditional integral viscosity measurements on a Münstedt-type extensional rheometer are combined with local measurements based on the in-situ visualization of the sample under extension. For elongational experiments at constant strain rates within a wide range of Weissenberg numbers (Wi), three distinct deformation regimes are identified. Corresponding to low values of Wi (regime I), the tensile stress displays a broad maximum, but such maximum is observed with various polymeric materials deformed at low rates and it should not be confused with the “viscosity overshoot” phenomenon. Corresponding to intermediate values of Wi (regime II), a local maximum of the integral extensional viscosity is systematically observed. Moreover, within this regime, a strong discrepancy between integral measurements and the space average of the local elongational viscosity is observed which indicates large deviations from an ideal uniaxial deformation process. Images of samples within this regime reinforce this finding by showing that, corresponding to the maximum of the integral viscosity, secondary necks develop along the sample. The emergence of a maximum of the integral elongational viscosity is, thus, related to the distinct inhomogeneity of deformation states and most probably not to the rheological properties of the material. In the fast stretching limit (high Wi, regime III), the overall geometric uniformity of the sample is well preserved, no secondary necks are observed and both the integral and the space averaged transient elongational viscosity show no maximum. A detailed but yet incomplete comparison of the experimental findings with results from the literature is presented and several open questions are stated.
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