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Article

Keywords:
spatial isotropy and anisotropy; heat equation; Lamé system; viscoelasticity; three-dimensional case; coupled system
Summary:
In this part we weaken the sufficient condition to obtain the stresses continuous and bounded in the threedimensional case, and we treat a certain coupled system.
References:
[1] J. Jarušek: On the regularity of solutions of a thermoelastic system under noncontinuous heating regimes. ApI. Mat. 35 (1990), 426-450. MR 1089924
[2] J. Jarušek: On the regularity of solutions of a thermoelastic system under noncontinuous heating regimes. Part II. Appl. Math. 36(1991), 161-180. MR 1109122
[3] J. Lions E. Magenes: Problèmes aux limites non-homogènes et applications. Dunod, Paris, 1968.
[4] J. Nečas: Dynamics of thermoelastic systems with strong viscosity. Proc. conf. part. diff. eq. Holzhau (GDR) 1988 (B. W. Schulze, ed.), Teubner Texte Math. Vol. 112, Leipzig, 1989.
[5] J. Nečas J. Jarušek J. Haslinger: On the solution of the variational inequality to the Signorini problem with small friction. Bol. Un. Mat. Ital. (5) 17-B (1980), 796-811. MR 0580559
[6] J. Nečas A. Novotný V. Šverák: Uniqueness of solutions to the systems for thermoelastic bodies with strong viscosity. Math. Nachr. 149 (1990), 319-324. DOI 10.1002/mana.19901490124 | MR 1124813
[7] J. Sprekels: Global solution in onedimensional magneto-thermoviscoelasticity. preprint, Univ. GH. Essen.
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