Elastic constitutive law with thermal effects for solid elements at variable temperature.
This law is used for a coupled thermo-mechanical analysis of elastic solids undergoing large strains.
Prepro: LELATH.F
Lagamine:
Plane stress state | YES |
Plane strain state | YES |
Axisymmetric state | YES |
3D state | NO |
Generalized plane state | YES |
Line 1 (2I5, 60A1) | |
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IL | Law number |
ITYPE | 200 |
COMMENT | Any comment (up to 60 characters) that will be reproduced on the output listing |
Line 1 (2I5) | |
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NTEMP | number of temperatures at which material data are given |
IENTH | = 1 to use the enthalpy formulation of the heat problem |
= 0 to use the classical formulation of the heat problem |
Repeat NTEMP times the definition of those parameters.
Line 1 (4G10.0) | |
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T | Temperature |
E | YOUNG's elastic modulus at temperature T |
ANU | POISSON's ratio at temperature T |
ALPHA | thermal expansion coefficient at temperature T |
Note that these values are tangent values (and not secant values).
Line 2 (1G10.0) | |
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RHO | Specific mass (used to take into account self-weight but only if the initial specific mass is constant) |
6 for 3D state
4 for the other cases
The stresses are the components of CAUCHY stress tensor in global (X,Y,Z) coordinates.
For the 3-D state:
SIG(1) | $\sigma_{xx}$ |
SIG(2) | $\sigma_{yy}$ |
SIG(3) | $\sigma_{zz}$ |
SIG(4) | $\sigma_{xy}$ |
SIG(5) | $\sigma_{xz}$ |
SIG(6) | $\sigma_{yz}$ |
For the other cases:
SIG(1) | $\sigma_{xx}$ |
SIG(2) | $\sigma_{yy}$ |
SIG(3) | $\sigma_{xy}$ |
SIG(4) | $\sigma_{zz}$ |
1
Q(1) | Element thickness (t) in plane stress state |
= 1 in plane strain state | |
Circumferential strain rate ($\dot{\varepsilon}_{\theta}$) in axisymmetric state | |
= 0 in 3-D state | |
element thickness (t) in generalized plane state |