elements:blz3d
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elements:blz3d [2019/03/04 10:01] admin |
elements:blz3d [2021/12/17 16:34] (current) laurent |
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| - | ====== BLZ3D ====== | + | ====== BLZ3D/BWD3D ====== |
| ===== Description ===== | ===== Description ===== | ||
| Line 6: | Line 6: | ||
| 8 node large strain volumetric element with hourglass and locking control. \\ | 8 node large strain volumetric element with hourglass and locking control. \\ | ||
| - | Implemented by: Zhu Yongyi, January 1992 | + | Implemented by: Zhu Yongyi, January 1992 \\ |
| + | Improved by: Laurent Duchêne and Pierre de Montleau, August 2004 (BWD3D version) | ||
| Type: 22 | Type: 22 | ||
| Prepro: BLZ3DA.F \\ | Prepro: BLZ3DA.F \\ | ||
| - | Lagamine: BLZ3DB.F\\ | + | Lagamine: BLZ3DB.F, BWD3DB.F\\ |
| ===== Input file ===== | ===== Input file ===== | ||
| - | |**Title** (A5) || | + | ^TITLE (A5)^^ |
| |TITLE | 'BLZ3D' in columns 1 to 5| | |TITLE | 'BLZ3D' in columns 1 to 5| | ||
| - | |**Control** (5I5) || | + | ^CONTROL (5I5)^^ |
| |NELEM | Number of elements | | |NELEM | Number of elements | | ||
| - | |INDPP |=0 if no weight (or no density if NTANA=-1)| | + | |INDPP |= 0 if no weight (or no density if NTANA=-1)| |
| - | |::: |=1 if weight taken into account (or density)| | + | |::: |= 1 if weight taken into account (or density)| |
| - | |INSHE |=0 for automatic calculation of shear locking parameter| | + | |INSHE |= 0 for automatic calculation of shear locking parameter| |
| - | |::: |=1 if shear coefficient taken into account| | + | |::: |= 1 if shear coefficient taken into account (see below)| |
| - | |::: |=-1 for use of element BWD3D (only 1 integration point)| | + | |::: |= -1 for use of element BWD3D (only 1 integration point)| |
| - | |ILOAX |=0 for global axis computation \\ ☛ Objectivity must be verified in the material law \\ ☛ No rotation of material axes| | + | |ILOAX |= 0 for global axis computation \\ ☛ Objectivity must be verified in the material law (with Jaumann correction)\\ ☛ No rotation of material axes| |
| - | |:::|<0 for computation with constant and symetrical velocity gradients \\ pseudo local axes : use of local axes on the time step but no evolution of the local axes on the following time step \\ ☛ Objectivity is verified \\ ☛ No rotation of material axes| | + | |:::|< 0 for computation with constant and symetrical velocity gradients \\ pseudo local axes : use of local axes on the time step but no evolution of the local axes on the following time step \\ ☛ Objectivity is verified \\ ☛ No rotation of material axes| |
| - | |:::|>0 for computation with local axes \\ ☛ Objectivity is verified \\ ☛ Rotation of material axes| | + | |:::|> 0 for computation with local axes \\ ☛ Objectivity is verified \\ ☛ Rotation of material axes| |
| - | |:::|units: \\ = | + | |:::|units: \\ = 1 for rotations incorporated in local tangent matrix :!: **Not available** \\ = 2 apply final rotation to local tangent matrix \\ = 3 apply initial rotation to local tangent matrix \\ = 4 compute tangent matrix through global perturbation method| |
| - | + | |:::|tens (only for ILOAX>0): \\ = 0 for local axes e<sub>1</sub>, e<sub>2</sub>, e<sub>3</sub> initially parallel to global axes e<sub>x</sub>, e<sub>y</sub>, e<sub>z</sub> \\ = 1 for local axes e<sub>1</sub>, e<sub>2</sub> given (and e<sub>3</sub>=e<sub>1</sub>∧e<sub>2</sub>) \\ = 2 for local axes e<sub>1</sub>, e<sub>2</sub> initially in the plane (e<sub>x</sub>, e<sub>y</sub>) forming an angle θ with e<sub>x</sub>, e<sub>y</sub> (and e<sub>3</sub>=e<sub>1</sub>∧e<sub>2</sub>)\\ = 3 same as 1 with different local axes for each element \\ = 4 same as 2 with different local axes for each element| | |
| + | |ISIG0| = 0 if no initial stresses| | ||
| + | |:::| = 1 for input of initial stresses| | ||
| + | ^CONSIDERATION OF WEIGHT (4G10.0) \\ Only if INDPP = 1 ^^ | ||
| + | |WSPE(1)| = specific weight in X direction| | ||
| + | |WSPE(2)| = specific weight in Y direction| | ||
| + | |WSPE(3)| = specific weight in Z direction| | ||
| + | |WSPE(4)| = density| | ||
| + | ^CONSIDERATION OF SHEAR LOCKING (1G10.0) \\ Only if INSHE = 1 ^^ | ||
| + | |PARSHE| Shear locking coefficient ∈ [0,1] \\ - close to 0: avoid shear locking but higher risk of hourglass modes (use for thin elements in flexion) \\ - close to 1: avoid hourglass modes but higher risk of shear locking (use for cubic elements in shear)| | ||
| + | ^INITIAL ORIENTATION OF LOCAL AXES (6G10.0) \\ Only if tens of ILOAX = 1 or 3 \\ (only one line if tens of ILOAX = 1, repeated for each element if tens of ILOAX = 3) ^^ | ||
| + | |e<sub>1</sub>(x)|coordinate of e<sub>1</sub> along e<sub>x</sub>| | ||
| + | |e<sub>1</sub>(y)|coordinate of e<sub>1</sub> along e<sub>y</sub>| | ||
| + | |e<sub>1</sub>(z)|coordinate of e<sub>1</sub> along e<sub>z</sub>| | ||
| + | |e<sub>2</sub>(x)|coordinate of e<sub>2</sub> along e<sub>x</sub>| | ||
| + | |e<sub>2</sub>(y)|coordinate of e<sub>2</sub> along e<sub>y</sub>| | ||
| + | |e<sub>2</sub>(z)|coordinate of e<sub>2</sub> along e<sub>z</sub>| | ||
| + | |Note: These vectors are normalized after reading but should be orthogonal: \\ e<sub>1</sub> • e<sub>2</sub> = e<sub>1</sub>(x) * e<sub>2</sub>(x) + e<sub>1</sub>(y) * e<sub>2</sub>(y) + e<sub>1</sub>(z) * e<sub>2</sub>(z) = 0|| | ||
| + | ^INITIAL ORIENTATION OF LOCAL AXES (1G10.0) \\ Only if tens of ILOAX = 2 or 4 \\ (only one line if tens of ILOAX = 2, repeated for each element if tens of ILOAX = 4)^^ | ||
| + | |THETA| Angle between e<sub>1</sub> and e<sub>x</sub> in degrees| | ||
| + | ^DEFINITION OF THE ELEMENTS (2I5/8I5/6G10)^^ | ||
| + | |NINTE| Number of integration points (1, 2, 4 or 8) \\ if NINTE = 1, add 40 to MVARI compared to maximum required by laws | | ||
| + | |LMATE| Number of the material law| | ||
| + | |NODES(8)| List of nodes| | ||
| + | |SIG0(6)| List of initial stresses (Only if ISIG0=1)| | ||
elements/blz3d.1551690063.txt.gz · Last modified: 2020/08/25 15:33 (external edit)
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