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Material functions generated by the complex viscosity
Authors:J. Stastna  D. De Kee
Affiliation:(1) Fluid Dynamics Research Institute, University of Windsor, N9B 3P4 Windsor, Ontario, Canada;(2) Department of Chemical Engineering, University of Windsor, N9B 3P4 Windsor, Ontario, Canada
Abstract:Based on the complex viscosity model various steady-state and transient material functions have been completed. The model is investigated in terms of a corotational frame reference. Also, BKZ-type integral constitutive equations have been studied. Some relations between material functions have been derived.C–1 Finger tensor - F[], (F–1[]) Fourier (inverse) transform - 
$$dot G$$
rate of deformation tensor in corotating frame - h(I, II) Wagner's damping function - Jagr(x) Bessel function - m parameter inh (I, II) - m(s) memory function - mk, nk integers (powers in complex viscosity model) - P int principal value of the integral - beta parameter in the complex viscosity model - 
$$dot gamma $$
rate of deformation tensor - 
$$dot gamma ,dot gamma _0 ,dot gamma _infty  $$
shear rates - gamma[],Gamma [] incomplete gamma function - Gamma (a) gamma function - 
$$eta (dot gamma )$$
steady-shear viscosity - eegr* complex viscosity - eegrprime, eegrPrime real and imaginary parts ofeegr* - eegr0 zero shear viscosity - eegr+, psgr1+ stress growth functions - eegr, psgr1- stress relaxation functions - psgr(s) relaxation modulus - psgr1(s) primary normal-stress coefficient - ø(a, b; z) degenerate hypergeometric function - lambda1, lambda2 time constants (parameters ofeegr*) - ohgr frequency - tau extra stress tensor
Keywords:Complex viscosity  relaxation modulus  material function  integral constitutive equation
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