2009
DOI: 10.1002/pen.21299
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Determination of polymeric medium flow rate in extruders based on a new correlation

Abstract: One of the most widespread practical methods of polymer processing is the extrusion method that is based on pressing a polymeric melt through channels of the molding tool which have different geometrical crosssections. The basic performance of extrusion is based on the pressure and flow performance which sets functional correlation between volumetric flow rate of a polymer medium, pressed through a molding tool, and created pressure drop. Arguments of this correlation are the rheological parameters of polymer … Show more

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Cited by 3 publications
(4 citation statements)
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“…For consideration both viscous and elastic properties of polymeric melts, following viscoelastic model is implemented [5, 14]. where $\overline \sigma$ denotes (::) stress tensor; P , Lagrange multiplier, determined by boundary condition; $\overline \delta$ , identity tensor; $\overline c$ , Cauchy strain tensor; ${\overline e}_{\rm {f}}$ , flow strain rate tensor; $\overline \omega$ , vortex tensor; $\overline e$ , strain rate tensor; θ 0 ( T ), relaxation time; G 0 ( T ), tensile modulus; W , strain energy function W = W ( I 1 , I 2 ); I 1 and I 2 , primary and secondary strain tensor invariants; ψ, dimensionless parameter $(\psi = 0\;{\rm{at}}\;\overline \omega = 0\;{\rm{and} }\psi = I\;{\rm{at}}\;\overline \omega \ne 0)$ ; f ( I 1 , I 2 ), dimensionless function that defines relaxation time, and $2W^{\rm S} = W(I_1, I_2 ) + W(I_2, I_1 )$ , symmetric function of W .…”
Section: Mathematical Descriptionmentioning
confidence: 99%
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“…For consideration both viscous and elastic properties of polymeric melts, following viscoelastic model is implemented [5, 14]. where $\overline \sigma$ denotes (::) stress tensor; P , Lagrange multiplier, determined by boundary condition; $\overline \delta$ , identity tensor; $\overline c$ , Cauchy strain tensor; ${\overline e}_{\rm {f}}$ , flow strain rate tensor; $\overline \omega$ , vortex tensor; $\overline e$ , strain rate tensor; θ 0 ( T ), relaxation time; G 0 ( T ), tensile modulus; W , strain energy function W = W ( I 1 , I 2 ); I 1 and I 2 , primary and secondary strain tensor invariants; ψ, dimensionless parameter $(\psi = 0\;{\rm{at}}\;\overline \omega = 0\;{\rm{and} }\psi = I\;{\rm{at}}\;\overline \omega \ne 0)$ ; f ( I 1 , I 2 ), dimensionless function that defines relaxation time, and $2W^{\rm S} = W(I_1, I_2 ) + W(I_2, I_1 )$ , symmetric function of W .…”
Section: Mathematical Descriptionmentioning
confidence: 99%
“…Most researchers use Mooney‐Rivlin potential, but there are differences between experimental and theoretical results for prediction of stress and strain. Results of recent research show that in various kinematical deformations, the following potential can be used [5]. …”
Section: Mathematical Descriptionmentioning
confidence: 99%
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