2022
DOI: 10.1002/zamm.202100533
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Generalized Moore‐Gibson‐Thompson thermoelastic fractional derivative model without singular kernels for an infinite orthotropic thermoelastic body with temperature‐dependent properties

Abstract: Many challenges in different applied fields of research, such as materials science, viscoelasticity, biological sciences, physics, and mechanical engineering, require the study of derivative operators using single singular or nonsingular kernels. Atangana and Baleanu (AB) constructed a novel fractional derivative without a singular kernel based on the extended Mittag–Leffler function to overcome the singular kernel problem seen in previous definitions of fractional‐order derivatives. In this article, we provid… Show more

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Cited by 16 publications
(8 citation statements)
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“…To demonstrate the numerical computations calculated using the proposed methodology, we consider the temperature-dependent thermoelastic smart nanomaterial properties of pure copper (Cu) nanoparticles [40,41] as shown in Table 1 and using the boundary conditions depicted in Figure 2 to exemplify the numerical computations computed by the suggested methodology. Under thermal and piezoelectric loadings, the considered thermoelastic smart nanomaterial deforms and becomes electrically polarized.…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…To demonstrate the numerical computations calculated using the proposed methodology, we consider the temperature-dependent thermoelastic smart nanomaterial properties of pure copper (Cu) nanoparticles [40,41] as shown in Table 1 and using the boundary conditions depicted in Figure 2 to exemplify the numerical computations computed by the suggested methodology. Under thermal and piezoelectric loadings, the considered thermoelastic smart nanomaterial deforms and becomes electrically polarized.…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…By using Kirchhoff transformation 𝑇= ( ) 𝑑Θ [30], Eq. ( 22) may be written as follows [31] ∇ 𝑇(𝐱, τ) + 1 𝜆 ℎ(𝐱, 𝑇, τ) = 𝜌 𝑐 𝜆 𝜕𝑇(𝐱, τ) 𝜕τ +𝑁𝑙 𝐱,𝑇,𝑇 (41) which can be expressed as [31] ∇ 𝑇(𝐱, τ) + 1 𝜆 ℎ 𝐱, 𝑇, 𝑇 ,τ = 𝜌 𝑐 𝜆 𝜕𝑇(𝐱, τ) 𝜕τ (42) in which…”
Section: Boundary Element Implementationmentioning
confidence: 99%
“…Fractional-order derivatives offer advantages over integer derivatives, providing more accurate mathematical and physical models for various technical issues [25][26][27]. Consequently, fractional NLSE models have become essential for understanding soliton dynamics in optical fibers, with various solution schemes developed over the past two decades [28][29][30][31][32][33][34][35][36][37][38][39]. The motivation behind this study stems from the growing need to address complex nonlinear phenomena across diverse scientific disciplines, particularly in optics and applied sciences.…”
Section: Introductionmentioning
confidence: 99%