F modeling ============== Characteristics of modeling ----------------------------------- We use a MEMBRANE modeling in large deformations (DEFORMATION =' GROT_GDEP ') with the Neo-Hookian law of behavior (RELATION =' ELAS_MEMBRANE_NH'). Bi-quadratic elements are used. Characteristics of the mesh ---------------------------- The mesh is the same as for C modeling. Tested sizes and results ------------------------------ The pressure applied during loading is tested. .. csv-table:: "**Identification**", "**Reference type**", "**Reference value**", "**Precision**" "Instant 0.1 - :math:`\mathit{ETA}\text{\_}\mathit{PILO}` ", "'SOURCE_EXTERNE'", "109.55 :math:`N/{m}^{2}` "," 8%" "Instant 0.2 - :math:`\mathit{ETA}\text{\_}\mathit{PILO}` ", "'SOURCE_EXTERNE'", "531.73 :math:`N/{m}^{2}` "," 2%" "Instant 0.3 - :math:`\mathit{ETA}\text{\_}\mathit{PILO}` ", "'SOURCE_EXTERNE'", "995.8 :math:`N/{m}^{2}` "," 2%" "Instant 0.4 - :math:`\mathit{ETA}\text{\_}\mathit{PILO}` ", "'SOURCE_EXTERNE'", "1276.2 :math:`N/{m}^{2}` "," 2%" "Instant 0.5 - :math:`\mathit{ETA}\text{\_}\mathit{PILO}` ", "'SOURCE_EXTERNE'", "1366.9 :math:`N/{m}^{2}` "," 0.7%" "Instant 0.6 - :math:`\mathit{ETA}\text{\_}\mathit{PILO}` ", "'SOURCE_EXTERNE'", "1344.7 :math:`N/{m}^{2}` "," 0.6%" "Instant 0.7 - :math:`\mathit{ETA}\text{\_}\mathit{PILO}` ", "'SOURCE_EXTERNE'", "1280.6 :math:`N/{m}^{2}` "," 0.4%" "Instant 0.8 - :math:`\mathit{ETA}\text{\_}\mathit{PILO}` ", "'SOURCE_EXTERNE'", "1203.0 :math:`N/{m}^{2}` "," 0.3%" "Instant 0.9 - :math:`\mathit{ETA}\text{\_}\mathit{PILO}` ", "'SOURCE_EXTERNE'", "1124.4 :math:`N/{m}^{2}` "," 0.1%" "Instant 1.0 - :math:`\mathit{ETA}\text{\_}\mathit{PILO}` ", "'SOURCE_EXTERNE'", "1049.0 :math:`N/{m}^{2}` "," 0.1%" .. image:: images/10000201000006CF00000512F0DBC90C32B5E7E4.png :width: 5.8098in :height: 4.3264in .. _RefImage_10000201000006CF00000512F0DBC90C32B5E7E4.png: Figure 6.2-a: Results of the D modeling vs numerical reference in figure :ref:`2.1 ` -a. notes --------- We used on-the-go piloting (SUIV_PILO) as for the D modeling. With bi-quadratic cells, therefore of a higher order than the reference solution, the results remain as satisfactory as with the quadratic cells of the E modeling.