Higher-order fractional constitutive equations of viscoelastic materials involving three different parameters and their relaxation and creep functions

Two higher-order fractional viscoelastic material models consisting of the fractional Voigt model (FVM) and the fractional Maxwell model (FMM) are considered. Their higher-order fractional constitutive equations are derived due to the models’ constructions. We call them the higher-order fractional constitutive equations because they contain three different fractional parameters and the maximum order of equations is more than one. The relaxation and creep functions of the higher-order fractional constitutive equations are obtained by Laplace transform method. As particular cases, the analytical solutions of standard (integer-order) quadratic constitutive equations are contained. The generalized Mittag–Leffler function and H-Fox function play an important role in the solutions of the higher-order fractional constitutive equations. Finally, experimental data of human cranial bone are used to fit with the models given by this paper. The fitting plots show that the models given in the paper are efficient in describing the property of viscoelastic materials.

[1]  Christian Friedrich Relaxation functions of rheological constitutive equations with fractional derivatives: Thermodynamical constraints , 1991 .

[2]  S. Welch,et al.  Application of Time-Based Fractional Calculus Methods to Viscoelastic Creep and Stress Relaxation of Materials , 1999 .

[3]  Mingyu Xu,et al.  Theoretical analysis of the velocity field, stress field and vortex sheet of generalized second order fluid with fractional anomalous diffusion , 2001 .

[4]  R. Bagley,et al.  A Theoretical Basis for the Application of Fractional Calculus to Viscoelasticity , 1983 .

[5]  T. Surguladze On Certain Applications of Fractional Calculus to Viscoelasticity , 2002 .

[6]  Tan Wen-chang,et al.  Representation of the constitutive equation of viscoelastic materials by the generalized fractional element networks and its generalized solutions , 2003 .

[7]  C. Friedrich Relaxation and retardation functions of the Maxwell model with fractional derivatives , 1991 .

[8]  Sunwoo Park Rheological modeling of viscoelastic passive dampers , 2001, SPIE Smart Structures and Materials + Nondestructive Evaluation and Health Monitoring.

[9]  T. Pritz Five-parameter fractional derivative model for polymeric damping materials , 2003 .

[10]  Yuriy A. Rossikhin,et al.  Analysis of the viscoelastic rod dynamics via models involving fractional derivatives or operators of two different orders , 2004 .

[11]  Nicole Heymans Constitutive equations for polymer viscoelasticity derived from hierarchical models in cases of failure of time-temperature superposition , 2003, Signal Process..

[12]  T. Atanacković A modified Zener model of a viscoelastic body , 2002 .

[13]  J. Martinez-vega,et al.  Modeling of the viscoelastic behavior of amorphous polymers by the differential and integration fractional method: the relaxation spectrum H(τ) , 2003 .

[14]  Ralf Metzler,et al.  ON THE RIEMANN-LIOUVILLE FRACTIONAL CALCULUS AND SOME RECENT APPLICATIONS , 1995 .

[15]  R. Metzler,et al.  Generalized viscoelastic models: their fractional equations with solutions , 1995 .

[16]  Y. Fung Foundations of solid mechanics , 1965 .

[17]  Ralf Metzler,et al.  Fractional relaxation processes and fractional rheological models for the description of a class of viscoelastic materials , 2003 .

[18]  W. Glöckle,et al.  A fractional model for mechanical stress relaxation , 1991 .

[19]  Igor Podlubny,et al.  The Laplace Transform Method for Linear Differential Equations of the Fractional Order , 1997, funct-an/9710005.

[20]  T. Nonnenmacher,et al.  Fractional integral operators and Fox functions in the theory of viscoelasticity , 1991 .

[21]  Arak M. Mathai,et al.  The H-function with applications in statistics and other disciplines , 1978 .