Abstract
A brief derivation of the equations for deformable dielectrics is presented. The basic theory generalises that due to Toupin [1], for it contains thermomechanical interactions and viscous dissipation within a non-equilibrium thermodynamic framework recently constructed by Bree and Beevers [2]. Some asymptotic and Lyapounov stability results are established for initial-boundary value problems in the linearised theory using extended energy arguments. Similar arguments are then applied to produce analogous stability results for small electro-mechanical perturbations superimposed on a large static deformation and a strong magnetic field. © 1981 Martinus Nijhoff Publishers.
Original language | English |
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Pages (from-to) | 241-256 |
Number of pages | 16 |
Journal | Applied Scientific Research |
Volume | 37 |
Issue number | 3-4 |
DOIs | |
Publication status | Published - Sept 1981 |