F modeling ============== Fluid behavior: THMC = LIQU_GAZ_ATMavec a constant saturation :math:`S=1` Characteristics of F modeling ------------------------------------- * Plane modeling * 1 mesh DPQ8 from the D_ PLAN_THM modeling: THM_ DPQ8 .. image:: images/100010E20000159A000013A3E04FB40CCC36EFED.svg :width: 288 :height: 288 .. _RefImage_100010E20000159A000013A3E04FB40CCC36EFED.svg: Tested sizes and results ------------------------------ Discretization in time: Several time steps (16) to study the evolution of pressure during the transition phase until it stabilizes. The time pattern is implicit (:math:`\theta =1`). List of calculation times in seconds: :math:`\mathrm{1,}\mathrm{5,}\mathrm{10,}\mathrm{50,}\mathrm{100,}\mathrm{500,}{10}^{3},{5.10}^{3},{10}^{4},5.{10}^{4},{10}^{5},5.{10}^{5},{10}^{6},5.{10}^{6},{10}^{7},{10}^{10}` The nodal fluid pressure unknowns evaluated in Code_Aster are variations from the initial reference pressures defined under the keyword THM_INIT, which is why this table shows pressure variations in our comparison between the Code_Aster calculation and the reference solution. .. csv-table:: "**Node/point**", "**Order Number**", "**Press**", "**Reference**" :math:`(\mathrm{Pa})` ", "**Tolerance** :math:`(\text{\%})`" ":math:`\mathrm{N1}/A` ", "1 (t=1 s)", ":math:`\mathrm{PRE1}` "," -3,98.10-2", "1.0" "", "2 (t=5s)", ":math:`\mathrm{PRE1}` "," -1,99.10-1", "1.0" "", "3 (t=10 s)", ":math:`\mathrm{PRE1}` "," -3,98.10-1", "1.0" "", "4 (t=50s)", ":math:`\mathrm{PRE1}` "," -1.99", "1.0" "", "8 (t=5.103s)", ":math:`\mathrm{PRE1}` "," -1,95.10+2", "1.0" "", "16 (t=1010s)", ":math:`\mathrm{PRE1}` "," -5.10+3", "1.0" ":math:`\mathrm{N3}/B` ", "1 (t=1 s)", ":math:`\mathrm{PRE1}` "," 3.98.10-2", "1.0" "", "2 (t=5s)", ":math:`\mathrm{PRE1}` ", "1,99.10-1", "1.0" "", "3 (t=10 s)", ":math:`\mathrm{PRE1}` ", "3,98.10-1", "2.0" "", "4 (t=50 s)", ":math:`\mathrm{PRE1}` ", "1.99", "2.0" "", "8 (t=5.103s)", ":math:`\mathrm{PRE1}` ", "1,95.10+2", "1.0" "", "16 (t=1010s)", ":math:`\mathrm{PRE1}` ", "5.10+3", "1.0" notes --------- Note that the pressures calculated for the two previous behaviors (THMC = LIQU_SATU (model :math:`E`) and THMC = LIQU_GAZ_ATM (model :math:`F`)) are equal in absolute values. The difference in signs is due to the fact that: * the pressure :math:`\mathrm{PRE1}` evaluated in the code is the water pressure for the behavior THMC = LIQU_SATU, * :math:`\mathrm{PRE1}` is equal to the capillary pressure for the behavior THMC = LIQU_GAZ. Capillary pressure is equal to the difference between gas pressure and liquid pressure. In the particular case where the dry air pressure is atmospheric pressure (THMC = LIQU_GAZ_ATM), the capillary pressure has the opposite value of the liquid pressure.