Constitutive law for mixed limit condition for element FMILC
This law is only used for non linear thermal analysis of solids. This constitutive law allows to impose a mixed limit condition on a boundary, with a classical penalty method.
Prepro: LFMILC.F
Plane stress state | YES |
Plane strain state | YES |
Axisymmetric state | YES |
3D state | YES |
Generalized plane state | YES |
Line 1 (2I5, 60A1) | |
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IL | Law number |
ITYPE | 124 |
COMMENT | Any comment (up to 60 characters) that will be reproduced on the output listing |
Line 1 (I5) | |
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IDDL | DDL number (3 = water, 4 = air, 5 = temperature, in 2D case) |
DDL number (4 = water, 5 = air, 6 = temperature, in 3D case) |
Line 1 (1G10.0) | |
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COEFK | K penalty coefficient |
1
SIG(1) | = output or input flow at the boundary : if $V_S < V_0$ : $q=0$ if $V_S > V_0$ : $q=K\left( V_0 - V_S \right) $ |
Where $V$ is either a pressure or a temperature, $V_0$ is the $V$ value of the environment node and $V_S$ is the V value of the integration point.
3
Q(1) | water pressure (IDDL= 3 (in 2D) or 4 (in 3D)) or gas pressure (IDDL= 4 (in 2D) or 5 (in 3D)) or temperature (IDDL= 5, (in 2D) or 6 (in 3D)) of the solid at the integration point under consideration (=$V_S$) |
Q(2) | reference water pressure (IDDL= 3 (in 2D) or 4 (in 3D)) or reference gas pressure (IDDL= 4 (in 2D) or 5 (in 3D)) or reference temperature (IDDL=5 (in 2D) or 6 (in 3D) (=$V_0$) |
Q(3) | = $q$ |