Reference problem ===================== Geometry --------- Lengths are expressed in meters. .. image:: images/Object_1.svg :width: 495 :height: 374 .. _RefImage_Object_1.svg: The cylindrical panel is embedded along its 4 sides and subjected to surface force. * given in the global frame of reference for modeling A: :math:`\mathrm{f}\mathrm{=}\mathrm{-}{f}_{z}{e}_{z};{f}_{z}>0` * given in the local coordinate system for modeling B: :math:`\mathrm{f}\mathrm{=}\mathrm{-}{f}_{z}n;{f}_{z}>0` which leads to membrane compression of the panel, accompanied by localized flexions. In the case of B modeling, :math:`n` is normal to the updated geometry of the panel. Because of the geometric and physical symmetry of the problem, only quarter :math:`{P}_{1}{P}_{2}{P}_{3}{P}_{4}` of the panel is modeled, taking into account symmetry conditions. Material properties ----------------------- Elastic behavior: :math:`E\mathrm{=}450000\mathit{MPa};\nu \mathrm{=}0.3` Boundary conditions and loads ------------------------------------- .. csv-table:: "Boundary conditions", ":math:`\mathrm{P2P3}`: :math:`\mathrm{DX}=0.` "," :math:`\mathrm{DY}=0.` "," "," :math:`\mathrm{DZ}=0.` "," :math:`\mathrm{DRX}=0` "," :math:`\mathrm{DRY}=0` "," :math:`\mathrm{DRZ}=0`" "", ":math:`\mathrm{P3P4}`: :math:`\mathrm{DX}=0.` "," :math:`\mathrm{DY}=0.` "," :math:`\mathrm{DZ}=0.` "," "," :math:`\mathrm{DRX}=0` "," :math:`\mathrm{DRY}=0` "," :math:`\mathrm{DRZ}=0`" "", "", "", "", "", "", "" "Symmetry:", ":math:`\mathrm{P1P2}`:", ":math:`\mathrm{DY}=0.` "," ", "", ":math:`\mathrm{DRX}=0.` ", "", ":math:`\mathrm{DRZ}=0.`" "", ":math:`\mathrm{P4P1}`: :math:`\mathrm{DX}=0.` ", "", "", "", "", ":math:`\mathrm{DRY}=0.` "," :math:`\mathrm{DRZ}=0.`" We look for the successive states of equilibrium under the load consisting of the surface force given in the global coordinate system: :math:`{f}_{z}(t)\mathrm{=}t` :math:`t` being the nickname. We are interested in the only vertical component of displacement in :math:`{P}_{1}`.