| ||||||||||||||
|
Plenary Lecture
Faculty of Applied Mathematical and Physical Sciences National Technical University of Athens Greece
The main characteristic of the linear Strain Gradient theory is the consideration of the existence of microstructure in the material, which in turn gives rise to a great amount of new independent kinematic variables. These new variables lead to complicated forms of main boundary value problem. For example, it is easy to verify that the equilibrium equations are of the 4th order with respect to the displacement field. Another, hindrance to the direct application of these theories is the fact that the complicated boundary conditions that appear in this framework are somewhat difficult to interpret physically. With the above in mind, various mixed formulations (of the Ciarlet-Raviart type) have been developed in order to incorporate combinations of variables that include, but do not limit to, the classic stress (ô) & strain (å), displacement field (u), double stress (ì), relative stress (ã) and 1st (è) & 2nd (k) gradient of the displacement field. For reasons of completeness the following mixed formulations are proposed 1) ì-ô-u 2) ì-u 3) ì-ô-k-å-u 4) è-u-ã. It should be noted that in this case a direct extension to the classic Hu – Washizu & Hellinger-Reissner energy functionals (as they appear in the standard elasticity), cannot be made due to the great plethora of viable combinations among the classic and microstructural kinematic variables. However, as it is shown in the present work, similar energy functionals can be stated due to the fact that all of the above stated mixed formulations originate from the form Another implication of the current work is that it can be seen as a broad reference base for future numerical implementations of these theories by means of, for instance, various weighted residual methods such as the Standard Galerkin method.
|
| |||||||||||||
| | | | ||||||||||||
| copyright - designed by WSEAS | ||||||||||||||