Abstract

In this work, an explicit solution of the initial-boundary value problem for a multidimensional time-fractional differential equation is constructed. The possibility of obtaining this equation from an integro-differential wave equation with a Mittag–Leffler–type memory kernel is shown. An explicit solution to the problem under consideration is obtained using the Laplace and Fourier transforms, the properties of the Fox H-functions and the convolution theorem.

Highlights

  • The presence of memory in such models indicates the dependence of its current state on a finite number of its previous states

  • This means the non-local properties of non-classical mathematical models, for example, in the mechanics of viscoelastic media when describing the action of aftereffect [1,2]

  • Fractional derivative operators have many definitions and have unique properties, but they all describe to one degree or another memory effect characterizing information about the previous states of the system

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Summary

Introduction to the Problem and Its Setting

The investigation of many mathematical models that have a fractal structure have numerous applied applications. The presence of memory in such models indicates the dependence of its current state on a finite number of its previous states This means the non-local properties of non-classical mathematical models, for example, in the mechanics of viscoelastic media when describing the action of aftereffect [1,2]. If the memory functions are given and are power-law, we can go to other types of equations that are based on derivatives of fractional orders, properties of which are considered in table books on fractional calculus [23]. Equation (1) for ρ = 1, m = 1 describes the anomalously diffusive transport of solute in heterogeneous porous media [27] This equation containing both the classical and fractional derivatives is more general and is of interest in the theory of the differential equations with fractional derivatives.

General Theories
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