Abstract
Although a complete unified theory for elasticity, plasticity, and damage does not yet exist, an approach on the basis of thermomechanical principles may be able to serve as the foundation for such a theory. With this in mind, as a first step, a mixed formulation is developed for fully coupled, spatially discretized linear thermoelasticity under the Lagrangian formalism by using Hamilton's principle. A variational integration scheme is then proposed for the temporal discretization of the resulting Euler-Lagrange equations. With this discrete numerical time-step solution, it becomes possible, for proper choices of state variables, to restate the problem in the form of an optimization. Ultimately, this allows the formulation of a principle of minimum generalized complementary potential energy for the discrete-time thermoelastic system.
| Original language | English |
|---|---|
| Pages (from-to) | 508-518 |
| Number of pages | 11 |
| Journal | Journal of Engineering Mechanics - ASCE |
| Volume | 138 |
| Issue number | 5 |
| DOIs | |
| State | Published - May 9 2012 |
Keywords
- Discrete variational calculus
- Flexibility methods
- Hamilton's principle
- Mixed Lagrangian formulation
- Mixed methods
- Symplectic algorithms
- Thermoelasticity
- Variational methods
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