Global sensitivity analysis of MGT thermo-magneto-microstretch media with reference-scaled thermal conductivity

This paper presents a theoretical and numerical investigation of the coupled thermo-magneto-elastic behavior of a microstretch thermoelastic half-space subjected to mechanical and magnetic loading within the Moore–Gibson–Thompson (MGT) theory of thermoelasticity. The thermal conductivity is modeled by the reference-temperature family 𝜅 = 𝜅 ⁢ ₀ ⁢ ( 1 − 𝛼 𝜅 ⁢ 𝑇 ⁢ ₀ ) , where 𝛼 𝜅 is a material parameter and 𝑇 ⁢ ₀ is the reference temperature. It is emphasized at the outset that this family assigns a constant conductivity to each realization when 𝑇 ⁢ ₀ and 𝛼 𝜅 are fixed; the model therefore belongs to the class of constant-property families rather than to evolving-temperature closures such as 𝜅 ⁡ ( 𝜃 ) = 𝜅 ⁡ ₀ ⁢ ( 1 + 𝐾 ⁢ ₁ ⁢ 𝜃 ) . The Kirchhoff transformation consequently reduces to the exact linear rescaling 𝜓 = ( 1 − 𝛼 𝜅 ⁢ 𝑇 ⁢ ₀ ) ⁢ 𝜃 , which introduces no thermal nonlinearity and does not alter the underlying material coupling constants. The governing system constitutive relations, the MGT heat-conduction equation, dimensionless field variables, normal-mode expansion, and associated boundary conditions is derived in full. The normal-mode solution is validated against four independent limiting cases: (i) 𝐻 ⁡ ₀ → 0 (non-magnetic thermo-microstretch), (ii) 𝛼 𝜅 → 0 (constant-conductivity MGT), (iii) suppression of microstretch (MGT thermoelastic half-space), and (iv) comparison with a published MGT half-space solution. A global sensitivity analysis (GSA) based on Sobol first- and total-order indices, the Morris elementary-effect method, and partial rank correlation coefficients (PRCC) is then performed on a parameter set drawn directly from the governing equations: 𝑋 = [ 𝑃 , 𝐻 ⁡ ₀ , 𝛼 𝜅 , 𝜏 ⁢ ₀ , 𝑘 ̄ , 𝜆 ⁢ ₀ , 𝛼 ⁢ ₀ ] ⁢ ᵀ . The results show that 𝛼 𝜅 dominates the response of nearly all quantities of interest, while the micropolar coupling k̄ and microstretch coupling 𝜆 ⁢ ₀ exert secondary but non-negligible influence. The magnetic parameter H₀ and the microstretch modulus α₀ have small total-order indices. The GSA is consistent with the mathematical structure of the formulation and identifies the parameters that most strongly control near-surface field amplification in MGT thermo-magneto-microstretch media.

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Journal
International Communications in Heat and Mass Transfer
Published
2026-10-14
DOI
https://doi.org/10.1016/j.icheatmasstransfer.2026.112858
Primary Topic
Thermoelastic and Magnetoelastic Phenomena
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article
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article

Global sensitivity analysis of MGT thermo-magneto-microstretch media with reference-scaled thermal conductivity

Sana Ben Moussa, Adnan Jahangir, Murat Yaylacı, Abdullah Yahya Abdullah Alzahrani et al.
International Communications in Heat and Mass Transfer
Thermoelastic and Magnetoelastic Phenomena
article

Global sensitivity analysis of MGT thermo-magneto-microstretch media with reference-scaled thermal conductivity

Sana Ben Moussa, Adnan Jahangir, Murat Yaylacı, Abdullah Yahya Abdullah Alzahrani, Maaz Ali Khan, Khulud Ziadi
article en

Abstract

This paper presents a theoretical and numerical investigation of the coupled thermo-magneto-elastic behavior of a microstretch thermoelastic half-space subjected to mechanical and magnetic loading within the Moore–Gibson–Thompson (MGT) theory of thermoelasticity. The thermal conductivity is modeled by the reference-temperature family 𝜅 = 𝜅 ⁢ ₀ ⁢ ( 1 − 𝛼 𝜅 ⁢ 𝑇 ⁢ ₀ ) , where 𝛼 𝜅 is a material parameter and 𝑇 ⁢ ₀ is the reference temperature. It is emphasized at the outset that this family assigns a constant conductivity to each realization when 𝑇 ⁢ ₀ and 𝛼 𝜅 are fixed; the model therefore belongs to the class of constant-property families rather than to evolving-temperature closures such as 𝜅 ⁡ ( 𝜃 ) = 𝜅 ⁡ ₀ ⁢ ( 1 + 𝐾 ⁢ ₁ ⁢ 𝜃 ) . The Kirchhoff transformation consequently reduces to the exact linear rescaling 𝜓 = ( 1 − 𝛼 𝜅 ⁢ 𝑇 ⁢ ₀ ) ⁢ 𝜃 , which introduces no thermal nonlinearity and does not alter the underlying material coupling constants. The governing system constitutive relations, the MGT heat-conduction equation, dimensionless field variables, normal-mode expansion, and associated boundary conditions is derived in full. The normal-mode solution is validated against four independent limiting cases: (i) 𝐻 ⁡ ₀ → 0 (non-magnetic thermo-microstretch), (ii) 𝛼 𝜅 → 0 (constant-conductivity MGT), (iii) suppression of microstretch (MGT thermoelastic half-space), and (iv) comparison with a published MGT half-space solution. A global sensitivity analysis (GSA) based on Sobol first- and total-order indices, the Morris elementary-effect method, and partial rank correlation coefficients (PRCC) is then performed on a parameter set drawn directly from the governing equations: 𝑋 = [ 𝑃 , 𝐻 ⁡ ₀ , 𝛼 𝜅 , 𝜏 ⁢ ₀ , 𝑘 ̄ , 𝜆 ⁢ ₀ , 𝛼 ⁢ ₀ ] ⁢ ᵀ . The results show that 𝛼 𝜅 dominates the response of nearly all quantities of interest, while the micropolar coupling k̄ and microstretch coupling 𝜆 ⁢ ₀ exert secondary but non-negligible influence. The magnetic parameter H₀ and the microstretch modulus α₀ have small total-order indices. The GSA is consistent with the mathematical structure of the formulation and identifies the parameters that most strongly control near-surface field amplification in MGT thermo-magneto-microstretch media.

International Communications in Heat and Mass TransferVol. 180
COMSATS University Islamabad (PK), Recep Tayyip Erdoğan University (TR), Umm al-Qura University (SA), Qurtuba University of Science and Information Technology (PK), University of Buner (PK), King Khalid University (SA)
Openalex Percentile: Top 23%
Thermoelastic and Magnetoelastic Phenomena
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