Carreau-Yasuda model

If some or all of this curve is present, the models used to fit the data are more complex and are of two types. The first of these is the Carreau-Yasuda model, in which the viscosity at a given point (T ) as well as the zero-shear and infinite-shear viscosities are represented. A Power Law index (mi) is also present, but is not the same value as n in the linear Power Law model. A second type of model is the Cross model, which has essentially the same parameters, but can be broken down into submodels to fit partial data. If the zero-shear region and the power law region are present, then the Williamson model can be used. If the infinite shear plateau and the power law region are present, then the Sisko model can be used. Sometimes the central power law region is all that is available, and so the Power Law model is applied (Figure H. 1.1.5). 

Basic Protocol 2 is for time-dependent non-Newtonian fluids. This type of test is typically only compatible with rheometers that have steady-state conditions built into the control software. This test is known as an equilibrium flow test and may be performed as a function of shear rate or shear stress. If controlled shear stress is used, the zero-shear viscosity may be seen as a clear plateau in the data. If controlled shear rate is used, this zone may not be clearly delineated. Logarithmic plots of viscosity versus shear rate are typically presented, and the Cross or Carreau-Yasuda models are used to fit the data. If a partial flow curve is generated, then subset models such as the Williamson, Sisko, or Power Law models are used (unithi.i). 

The models used are typically either the Cross model or the Carreau-Yasuda model (UNIT Hl.l), if a complete curve is generated. A complete curve has both plateaus present (zero and infinite shear see Figure HI.1.4). 

The Bird-Carreau-Yasuda Model. A model that fits the whole range of strain rates was developed by Bird and Carreau [7] and Yasuda [72] and contains five parameters ... 

In order to parameterize the data into a descriptive model, the combined data sets of viscosity and shear rate relationship for linear and linear-branched PLA are fitted to the Carreau—Yasuda model. The form of the model used is given by (Lehermeier and Dorgan 2001) ... 

Figure 4 illustrates how the Carreau-Yasuda model meets the shear viscosity data of Fig. 2. A non-linear fitting algorithm (i.e. Marquardt-Levenberg) was used to obtain the parameters given in the inset. As can be seen the fit curve provides a shear viscosity function that corresponds reasonably well with experimental data so that the high shear behavior is asymptotic to a power law and the very low shear behavior corresponds to the pseudo-Newtonian viscosity po- The characteristic time X (56.55 s) can be considered as the reverse of a critical shear rate (i.e. = Yc = 0.0177 s ) that corresponds to the intersection between the high shear power...

Fig. 4 Shear viscosity function of an unfilled SBR1500 compound at 100 °C as fitted with the Carreau-Yasuda model see Fig. 1 for symbols meaning...

An attractive mathematical model for such a dynamic viscosity function is again the Carreau-Yasuda model, i.e. ... 

Fig. 9 Dynamic Viscosity function of gum EPDM2504 at 100 °C authors s experimental data and fitted Carreau-Yasuda model...

During the experiments, the solid concentration was increased to 20% by volume. Except for suspensions with plastic particles, the suspensions showed a Newtonian behavior up to volume contents of 15 %. Suspensions with glass beads and s = 0.2 as well as all examined suspensions with plastic particles showed a shear thinning behavior. Considering the non-Newtonian behavior of these suspensions in the calculation of the time steady flow based on Eqs. (5.9-5.21), the viscosity of the suspension had to be described by a model depending on the deformation speed y. A Carreau-Yasuda model according to Eq. (5.52) fitted well to measurements carried out with a Couette system. The parameters Hq, a, n, and X were determined by the rheological measurements. 

We then simulate shape oscillations of shear-thinning droplets. At first the implementation of the Carreau-Yasuda model is validated against experimental data. We then analyze the droplet oscillations and compare them to Newtonian droplets with the same Ohnesorge number. We investigate the viscosity distribution... 

C.1 Carreau-Yasuda Model Parameters from Regression Analysis. Use either Solve in Excel or the IMSL subroutine RNLIN (Example 2.1) to find the Carreau-Yasuda model parameters [Eq. 2.8 with (n — l)/2 replaced with (n - )/a] for LLDPE at 170 °C (viscosity data are given in Appendix A.3) and compare the results with those given in Table 2.1. 

A6.4.8 Fitting the Virgin Polystyrene Data with the Carreau-Yasuda Model... 

Figure 2.16 Shear-dependent viscosity of poly(styrene) melt at 453 K, estimated from the Carreau-Yasuda model.

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