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Representation of the rheological properties of polymer melts in terms of complex fluidity
Authors:V Verney  A Michel
Institution:(1) C.N.R.S., Laboratoire des Matériaux Organiques, BP. 24, F-69390 Vernaison, France
Abstract:In dynamic rheological experiments melt behavior is usually expressed in terms of complex viscosityepsi * (ohgr) or complex modulusG * (ohgr). In contrast, we attempted to use the complex fluidityphiv * (ohgr) = 1/µ * (ohgr) to represent this behavior. The main interest is to simplify the complex-plane diagram and to simplify the determination of fundamental parameters such as the Newtonian viscosity or the parameter of relaxation-time distribution when a Cole-Cole type distribution can be applied. epsi * (ohgr) complex shear viscosity - epsiprime(ohgr) real part of the complex viscosity - epsiPrime(ohgr) imaginary part of the complex viscosity - G * (ohgr) complex shear modulus - Gprime(ohgr) storage modulus in shear - GPrime(ohgr) loss modulus in shear - J * (ohgr) complex shear compliance - Jprime(ohgr) storage compliance in shear - JPrime(ohgr) loss compliance in shear - gamma shear strain - 
$$\dot \gamma $$
rate of strain - ohgr angular frequency (rad/s) - tau shear stress - delta loss angle - phiv * (ohgr) complex shear fluidity - phivprime(ohgr) real part of the complex fluidity - phivPrime(ohgr) imaginary part of the complex fluidity - epsi 0 zero-viscosity - lambda 0 average relaxation time - h parameter of relaxation-time distribution
Keywords:Melt rheology  complexviscosity  complexfluidity  polypropylene  polyethylene  polystyrene
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