Abstract

This article constructs a mathematical model based on fractional-order deformations for a one-dimensional, thermoelastic, homogenous, and isotropic solid sphere. In the context of the hyperbolic two-temperature generalized thermoelasticity theory, the governing equations have been established. Thermally and without deformation, the sphere’s bounding surface is shocked. The singularities of the functions examined at the center of the world were decreased by using L’Hopital’s rule. Numerical results with different parameter fractional-order values, the double temperature function, radial distance, and time have been graphically illustrated. The two-temperature parameter, radial distance, and time have significant effects on all the studied functions, and the fractional-order parameter influences only mechanical functions. In the hyperbolic two-temperature theory as well as in one-temperature theory (the Lord-Shulman model), thermal and mechanical waves spread at low speeds in the thermoelastic organization.

Highlights

  • Academic Editor: Nicholas Alexander is article constructs a mathematical model based on fractional-order deformations for a one-dimensional, thermoelastic, homogenous, and isotropic solid sphere

  • In the hyperbolic two-temperature theory as well as in one-temperature theory, thermal and mechanical waves spread at low speeds in the thermoelastic organization

  • E thermoelasticity model has been developed by Chen and Gurtin, based on two different conductive and dynamic temperatures. e temperature differential is proportionate to the heat source [1]

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Summary

Introduction

Academic Editor: Nicholas Alexander is article constructs a mathematical model based on fractional-order deformations for a one-dimensional, thermoelastic, homogenous, and isotropic solid sphere. Numerical results with different parameter fractional-order values, the double temperature function, radial distance, and time have been graphically illustrated.

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