4.7 Article

Incorporating Rheological Nonlinearity into Fractional Calculus Descriptions of Fractal Matter and Multi-Scale Complex Fluids

期刊

FRACTAL AND FRACTIONAL
卷 5, 期 4, 页码 -

出版社

MDPI
DOI: 10.3390/fractalfract5040174

关键词

Fractional Maxwell Model; non-linear fractional viscoelasticity; Wagner model; damping functions; rate-dependent steady shear viscosity; Gamma function

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This paper applies ideas from fractional calculus to study the rheological response of soft materials under steady-shearing flow conditions, focusing on linear viscoelastic and non-linear response characteristics. By incorporating damping functions with fractional viscoelastic constitutive models, an analytical framework is developed to calculate material properties such as rate-dependent shear viscosity. Through analytical and computational evaluations of shear viscosity, the study shows that the observed shear-thinning behavior is influenced by the damping function used, with different forms leading to differing power-law responses.
In this paper, we use ideas from fractional calculus to study the rheological response of soft materials under steady-shearing flow conditions. The linear viscoelastic properties of many multi-scale complex fluids exhibit a power-law behavior that spans over many orders of magnitude in time or frequency, and we can accurately describe this linear viscoelastic rheology using fractional constitutive models. By measuring the non-linear response during large step strain deformations, we also demonstrate that this class of soft materials often follows a time-strain separability principle, which enables us to characterize their nonlinear response through an experimentally determined damping function. To model the nonlinear response of these materials, we incorporate the damping function with the integral formulation of a fractional viscoelastic constitutive model and develop an analytical framework that enables the calculation of material properties such as the rate-dependent shear viscosity measured in steady-state shearing flows. We focus on a general subclass of fractional constitutive equations, known as the Fractional Maxwell Model, and consider several different analytical forms for the damping function. Through analytical and computational evaluations of the shear viscosity, we show that for sufficiently strong damping functions, for example, an exponential decay of fluid memory with strain, the observed shear-thinning behavior follows a power-law response with exponents that are set by the power-law indices of the linear fractional model. For weak damping functions, however, the power-law index of the high shear rate viscosity is set by the terminal behavior of the damping function itself at large strains. In the limit of a very weak damping function, the theoretical formulation predicts an unbounded growth of the shear stress with time and a continuously growing transient viscosity function that does not converge to a meaningful steady-state value. By determining the leading terms in our analytical solution for the viscosity at both low and high shear rates, we construct an approximate analytic expression for the rate-dependent viscosity. An error analysis shows that, for each of the damping functions considered, this closed-form expression is accurate over a wide range of shear rates.

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