Introduction ==== Geometry ---- The study concerns a thick steel plate. Its geometry is simple. It is a simple flattened cube with the following dimensions [cf. :numref:`geometrie-vue-3D`]: * length = :math:`\mathrm{2,0}` meters; * width = :math:`\mathrm{2,0}` meters; * thickness = :math:`\mathrm{0,003}` meters. The plate is firmly embedded on one of its sides (ENCAS) and fixed on a vibrating table. We want to calculate the displacement of a point located on the upper face in a corner of a plate, opposite to the embedment (point P). .. figure:: images/geometrie_vue_3D.png :name: geometrie-vue-3D :width: 5.4917in :height: 2.672in Geometry (3D view) .. figure:: images/geometrie_vue_dessus.png :width: 3.998in :height: 2.8354in :name: geometrie-vue-dessus Geometry (top view) Materials ---- For linear analyses, steel is considered to be an isotropic, linear elastic material: * Young's modulus: :math:`E\mathrm{=}200000.{10}^{+6}\mathit{Pa}`; * Poisson's ratio: :math:`\nu \mathrm{=}\mathrm{0,3}`; * density: :math:`\rho \mathrm{=}8000\mathit{kg}\mathrm{/}{m}^{3}`. Post-elastic (plastic) behavior is idealized by an elastoplastic law with linear work hardening whose plastic modulus (the plastic slope) is 1\% of the elastic Young's modulus. The elastic stress threshold is 200 MPa. Boundary conditions and loading ---- The plate is embedded on one of its sides. A distracted (or somewhat facetious) engineer made a mistake in the vibrating table settings. Instead of the expected stress (a synthetic accelerogram), it sent a simple sinusoidal signal but of very high amplitude. The plate was not designed for such a shock and an attempt is being made to determine the movement that the plate may have undergone during this unfortunate test. The input signal is a simple sine with frequency :math:`15\mathit{Hz}`. The amplitude is :math:`\mathrm{30g}` horizontally and :math:`\mathrm{30g}` vertically downwards (:math:`g=10m/{s}^{2}`). The duration of the signal is :math:`0.5s`.