Two-phase saturated porous elements with water displacement dof (u-U elements)
Similar to the u-p elements, these elements are implemented for simulating the response of a two-phase solid-fluid fully coupled material, based on Biot's theory of porous medium:
- The porous medium is composed of one solid phase (e.g. soil skeleton) and one pore-fluid (e.g. water) and is assumed to be always saturated.
-
Each node has 4 (6 in 3D) degrees of freedom:
- solid displacements \(u_1\) and \(u_2\) (and \(u_3\) in 3D)
- water displacements \(w_1\) and \(w_2\) (and \(w_3\) in 3D)
-
The prescribed densities are the density of the solid grains \(\rho^s\) and the pore fluid \(\rho^w\). The density of the continuum \(\rho\) is calculated based on the assigned porosity \(n\) (or void ratio):
$$ \rho = (1-n) \cdot \rho^s + n \cdot \rho^w $$
2D Elements
Element label | Dim. | Shape | Nodes | Interpolation Order | nIP* | Remarks |
---|---|---|---|---|---|---|
u4u4 |
2D | rectangle | 4 | linear | 4 | (1) |
u4u4-red |
2D | rectangle | 4 | linear | 1 | (2) |
u8u8 |
2D | rectangle | 8 | quadratic | 9 | (1) |
u8u8-red |
2D | rectangle | 8 | quadratic | 1 | (2) |
Axisymmetric Elements
Element label | Dim. | Shape | Nodes | Interpolation Order | nIP* | Remarks |
---|---|---|---|---|---|---|
u4u4-ax |
axisym | rectangle | 4 | linear | 4 | (1) |
u4u4-ax-red |
axisym | rectangle | 4 | linear | 1 | (2) |
u8u8-ax |
axisym | rectangle | 8 | quadratic | 9 | (1) |
u8u8-ax-red |
axisym | rectangle | 8 | quadratic | 1 | (2) |
3D Elements
Element label | Dim. | Shape | Nodes | Interpolation Order | nIP* | Remarks |
---|---|---|---|---|---|---|
u8u8-3d |
3D | brick | 8 | linear | 8 | (1) |
u8u8-3d-red |
3D | brick | 8 | linear | 1 | (2) |
u20u20 |
3D | brick | 20 | quadratic | 27 | (1), (3) |
Remarks
* | nIP = number of integration points |
---|---|
(1) | Due to the full integration, the element will behave badly for isochoric material behavior. This shortcoming is more pronounced for linear interpolated elements and less pronounced for quadratic interpolated ones. |
(2) | Reduced integration: This element does not suffer from the same locking issues as fully integrated elements, however, due to the rank deficiency of the element stiffness matrix, a Hourglass stiffness has to be applied to prevent spurious zero-energy modes. For more information see *Material, *Hourglass and the Theory Manual. |
(3) | 3D-serendipity elements such as the element are not suitable for contact analysis. The option bi-quadratic , however, can not be used for u20u20 elements! |
For u-U elements it is strongly recommended to use reduced integration.
Notice that these elements require the definition of a two-phase material: (*Material,..., Phases=2
) as described in *Material.