Continuous dependence and convergence for a Moore-Gibson-Thompson thermoelastic problem

In this article, we investigate how the solutions of the Moore-Gibson-Thompson thermoelasticity vary after a change of the relaxation parameter or the conductivity rate parameter, although, in the second case, only for radial solutions. The results focus on the structural stability. We also obtain t...

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Detalles Bibliográficos
Autores: Fernández García, José Ramón|||0000-0002-8533-1858, Pellicer Sabadí, Marta|||0000-0003-4107-6610, Quintanilla de Latorre, Ramón|||0000-0001-7059-7058
Tipo de recurso: artículo
Fecha de publicación:2024
País:España
Institución:Universitat Politècnica de Catalunya (UPC)
Repositorio:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglés
OAI Identifier:oai:upcommons.upc.edu:2117/401907
Acceso en línea:https://hdl.handle.net/2117/401907
https://dx.doi.org/10.1080/15397734.2023.2246535
Access Level:acceso abierto
Palabra clave:Thermoelasticity
Continuous dependence
Convergence
Structural stability
Energy arguments
MGT thermoelasticity
Termoelasticitat
Àrees temàtiques de la UPC::Matemàtiques i estadística::Matemàtica aplicada a les ciències
Descripción
Sumario:In this article, we investigate how the solutions of the Moore-Gibson-Thompson thermoelasticity vary after a change of the relaxation parameter or the conductivity rate parameter, although, in the second case, only for radial solutions. The results focus on the structural stability. We also obtain the convergence of the Moore-Gibson-Thompson thermoelasticity to the type III thermoelasticity and the convergence of the Moore-Gibson-Thompson thermoelasticity to the Lord-Shulman thermoelasticity in the case of radial solutions. For the structural stability results, a certain measure for the difference of solutions can be used to control by an expression depending on the square of the difference of the parameters, and, for the convergence results, a measure of the difference of the solutions is proved to be controlled by the square of the vanishing parameter. In the proof of the above results, the energy arguments are used. It is worth saying that there are no results of this kind for the Moore-Gibson-Thompson thermoelasticity. Therefore, our results are the first contributions in this sense