Citation: Abbas, I.; Marin, M.;
Hobiny, A.; Vlase, S. Thermal
Conductivity Study of an Orthotropic
Medium Containing a Cylindrical
Cavity. Symmetry 2022, 14, 2387.
https://doi.org/10.3390/
sym14112387
Academic Editors: Vasilis K.
Oikonomou and Victor A. Eremeyev
Received: 29 September 2022
Accepted: 8 November 2022
Published: 11 November 2022
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symmetry
S S
Article
Thermal Conductivity Study of an Orthotropic Medium
Containing a Cylindrical Cavity
Ibrahim Abbas
1,2
, Marin Marin
3,
* , Aatef Hobiny
2
and Sorin Vlase
3,4,
*
1
Mathematics Department, Faculty of Science, Sohag University, Sohag 82524, Egypt
2
Mathematics Department, Faculty of Science, King Abdulaziz University, Jeddah 21521, Saudi Arabia
3
Department of Mathematics and Computer Science, Transilvania University of Brasov,
500036 Brasov, Romania
4
Romanian Academy of Technical Sciences, B-dul Dacia 26, 030167 Bucharest, Romania
* Correspondence: m.marin@unitbv.ro (M.M.); svlase@unitbv.ro (S.V.)
Abstract: An interesting feature that appears in the thermoelastic interaction in an orthotropic
material containing cylindrical cavities is addressed in this study. For this purpose, the Finite
Element Method is applied to analyze a generalized thermoelasticity theory with a relaxation time.
For the development of the model, a thermal conductivity that is dependent on the temperature
of the orthotropic medium was considered. The boundary condition for the internal surface of
a cylindrical hollow is defined by the thermal shocks and the traction on the free surface. The
nonlinear formulations of thermoelastic based on thermal relaxation time in orthotropic mediums
are abbreviated using the Finite Element Method. The nonlinear equations without Kirchhoff’s
transformations are presented. The results are graphically represented to demonstrate how changing
thermal conductivity affects all physical values.
Keywords: thermal relaxation; orthotropic medium; cylindrical cavity; FEM; constitutive law
1. Introduction
In solid mechanics and material science, an orthotropic media possesses material
properties at specified points that change along the three perpendicular axes, each having
twofold rotational symmetry. Over the last four decades, a number of mathematicians
and engineers have exhibited a great deal of interest in generalized thermoelastic theories
because of their remarkable realistic implications in a range of domains, such as acoustics,
continuum mechanic, nuclear engineering, aeronautic, high-energy particle accelerator,
and so on.
Biot [1] developed the coupled thermoelastic hypothesis to overcome the inconsis-
tency appearing by the uncoupled hypothesis. In this theory, the heat transport and
elasticity formulations are coupled. Lord and Shulman [2] proposed many extensions of
the thermoelastic theory. In 1980, Dhaliwal and Sherief [3] modified the Lord and Shul-
man model to include anisotropic cases. Singh [4] has explored the wave propagation in
porous materials using thermoelastic models in general. Alesemi [5] used the LS model
under the influence of centrifugal force and Coriolis to investigate the plane waves in
magneto-thermoelasticity anisotropic materials. Marin et al. [6] presented some results
in the Green and Lindsay model of thermoelastic structures. Aboueregal et al. [7] have
studied the effects of varying properties and rotations in visco-thermoelastic orthotropic
cylinders. Biswas [8] studied the surface waves in porous nonlocal orthotropic thermoe-
lastic materials. Abd-Alla et al. [9–11] have discussed the propagations of Rayleigh wave
in a generalized thermo-magneto-elasticity orthotropic medium under gravity field with
initial stresses. Biswas and Mukhopadhyay [12] have used the eigenfunction expansion
approach to analyze thermal shocks behaviors in thermoelastic orthotropic media by using
three thermoelastic models with a magnetic field. Demirdži´ c et al. [13] have applied the
Symmetry 2022, 14, 2387. https://doi.org/10.3390/sym14112387 https://www.mdpi.com/journal/symmetry