We consider a thermoelastic theory where the heat conduction is described by the Moore–Gibson–Thompson equation. In fact, this equation can be obtained after the introduction of a relaxation parameter in the Green–Naghdi type III model. We analyse the one- and three-dimensional cases. In three dimensions, we obtain the well-posedness and the stability of solutions. In one dimension, we obtain the exponential decay and the instability of the solutions depending on the conditions over the system of constitutive parameters. We also propose possible extensions for these theories.
ConejeroJALizamaCRódenasF. Chaotic behaviour of the solutions of the Moore–Gibson–Thompson equation. Appl Math Informat Sci2005; 9: 2233–2238.
2.
KaltenbacherBLasieckaIMarchandR. Wellposedness and exponential decay rates for the Moore–Gibson–Thompson equation arising in high intensity ultrasound. Control Cybernet2011; 40: 971–988.
3.
LasieckaIWangX. Moore–Gibson–Thompson equation with memory, part II: General decay of energy. J Diff Eqns2015; 259: 7610–7635.
4.
MarchandRMcDevittTTriggianiR. An abstract semigroup approach to the third order Moore–Gibson–Thompson partial differential equation arising in high-intensity ultrasound: structural decomposition, spectral analysis, exponential stability. Math Meth Appl Sci2012; 35: 1896–1929.
5.
PellicerMSaid-HouariB. Wellposedness and decay rates for the Cauchy problem of the Moore–Gibson–Thompson equation arising in high intensity ultrasound. Appl Math Optimiz2017. DOI: 10.1007/s00245-017-9471-8
6.
PellicerMSola-MoralesJ. Optimal scalar products in the Moore–Gibson–Thompson equation. Evol Eq Control Theory2019; 8: 203–220.
7.
ThompsonPA. Compressible-Fluid Dynamics. New York: McGraw-Hill, 1972.
8.
CattaneoC. On a form of heat equation which eliminates the paradox of instantaneous propagation. C R Acad Sci Paris1958; 247: 431–433.
9.
LordHWShulmanY. A generalized dynamical theory of thermoelasticity. J Mech Phys Solids1967; 15: 299–309.
10.
ChandrasekharaiahDS. Hyperbolic thermoelasticity: A review of recent literature. Appl Mech Rev1998; 51: 705–729.
HetnarskiRBIgnaczakJ. Nonclassical dynamical thermoelasticity. Int J Solids Struct2000; 37: 215–224.
13.
IgnaczakJOstoja-StarzewskiM. Thermoelasticity with Finite Wave Speeds (Oxford Mathematical Monographs). Oxford: Oxford University Press, 2010.
14.
RackeR. Asymptotic behavior of solutions in linear 2- or 3-D thermoelasticity with second sound. Quart Appl Math2003; 61: 315–328.
15.
RackeR. Thermoelasticity with second sound - exponential stability in linear and non-linear 1-D. Math Meth Appl Sci2002; 25: 409–441.
16.
GreenAENaghdiPM. On undamped heat waves in an elastic solid. J Therm Stress1992; 15: 253–264.
17.
GreenAENaghdiPM. Thermoelasticity without energy dissipation. J Elasticity1993; 31: 189–208.
18.
GreenAENaghdiPM. A unified procedure for contruction of theories of deformable media. I. Classical continuum physics. Proc R Soc Lond A1995; 448: 335–356.
19.
GreenAENaghdiPM. A unified procedure for contruction of theories of deformable media. II. Generalized continua. Proc R Soc Lond A1995; 448: 357–377.
20.
GreenAENaghdiPM. A unified procedure for contruction of theories of deformable media. III. Mixtures of interacting continua. Proc R Soc Lond A1995; 448: 379–388.
21.
GiorgiCGrandiDPataV. On the Green–Naghdi type III heat conduction model. Discrete Continuous Dynam Syst B2014; 19: 2133–2143.
22.
LiuYLinYLiY. Convergence result for the thermoelasticity of type III. Appl Math Lett2013; 26: 97–102.
23.
LiuZQuintanillaR. Analiticity of solutions in type III thermoelastic plates. IMA J Appl Math2010; 75: 637–646.
24.
KothariSMukhopadhyayS. Study of harmonic plane waves in rotating thermoelastic media of type III. Math Mech Solids2012; 17: 824–839.
25.
MukhopadhyaySKumarR. A problem of thermoelastic interactions in an infinite medium with a cylindrical hole in generalized thermoelasticity III. J Therm Stress2008; 31: 455–475.
26.
MagañaAQuintanillaR. Exponential stability in type III thermoelasticity with microtemperatures. Z Angew Math Phys2018; 69(5): 129(1)–129(8).
27.
MiranvilleAQuintanillaR. Some generalizations of the Caginalp phase-field system. Applicable Anal2009; 88: 877–894.
28.
MiranvilleAQuintanillaR. A type III phase-field system with logarithmic potential. Appl Math Lett2011; 24: 1003–1008.
29.
MiranvilleAQuintanillaR. Exponential stability in type III thermoelasticity with voids. Appl Math Lett2019; 94: 30–37.
30.
MukhopadhyaySPrasadRKumarR. Variational and reciprocal principles in linear theory of type-III thermoelasticity. Math Mech Solids2011; 16: 435–444.
31.
QuintanillaR. Structural stability and continuous dependence of solutions in thermoelasticity of type III. Discrete Continuous Dynam Syst B2001; 1: 463–470.
32.
QuintanillaR. Convergence and structural stability in thermoelasticity. Appl Math Computat2003; 135: 287–300.
33.
QuintanillaRStraughanB. Growth and uniqueness in thermoelasticity. Proc R Soc Lond A2000; 455: 1429.
34.
StraughanB. Heat waves. Appl Math Sci2011; 177, New York: Springer.
35.
RenardyMHrusaWJNohelJA. Mathematical Problems in Viscoelasticity. London: Longman Scientific and Technical, 1987.
36.
MagañaAQuintanillaR. On the existence and uniqueness in phase-lag thermoelasticity. Meccanica2018; 53: 125–134.
37.
ChoudhuriSKR. On a thermoelastic three-phase-lag model. J Therm Stress2007; 30: 231–238.
38.
PazyA. Semigroups of linear operators and applications to partial differential equations. Appl Math Sci1983; 44, Berlin: Springer.
39.
LiuZZhengS. Semigroups Associated With Dissipative Systems (Chapman & Hall/CRC Research Notes in Mathematics, Vol. 398). Boca Raton, FL: Chapman & Hall/CRC, 1999.
40.
QuintanillaR. A condition on the delay parameters in the one-dimensional dual-phase-lag thermoelastic theory. J Therm Stress2003; 26: 713–721.