SHELL281
8-Node
Structural Shell
SHELL281 Element Description
SHELL281 is suitable for analyzing thin to moderately-thick shell structures. The element has eight nodes with six degrees of freedom at each node: translations in the x, y, and z axes, and rotations about the x, y, and z-axes. (When using the membrane option, the element has translational degrees of freedom only.)
SHELL281 is well-suited for linear, large rotation, and/or large strain nonlinear applications. Change in shell thickness is accounted for in nonlinear analyses. The element accounts for follower (load stiffness) effects of distributed pressures.
SHELL281 may be used for layered applications for modeling composite shells or sandwich construction. The accuracy in modeling composite shells is governed by the first-order shear-deformation theory (usually referred to as Mindlin-Reissner shell theory).
The element formulation is based on logarithmic strain and true stress measures. The element kinematics allow for finite membrane strains (stretching). However, the curvature changes within a time increment are assumed to be small.
See SHELL281 for more details about this element.
SHELL281 Input Data
The following figure shows the geometry, node locations, normal direction, and multilayer construction for this element. The element is defined by shell section information and by eight nodes (I, J, K, L, M, N, O and P).
Midside nodes may not be removed from this element. See Quadratic Elements (Midside Nodes) in the Modeling and Meshing Guide for more information about the use of midside nodes.
A triangular-shaped element may be formed by defining the same node number for nodes K, L and O.
Single-Layer Definition
To define the thickness (and other information), use section definition, as follows:
A single-layer shell section definition provides flexible options. For example, you can specify the number of integration points used and the material orientation.
Multilayer Definition
The shell section commands allow for layered shell definition. Options are available for specifying the thickness, material, orientation, and number of integration points through the thickness of the layers.
You can designate the number of integration points (1, 3, 5, 7, or 9) located through the thickness of each layer when using section input. When only one, the point is always located midway between the top and bottom surfaces. If three or more points, two points are located on the top and bottom surfaces respectively and the remaining points are distributed at equal distances between the two points. The default number of integration points for each layer is three; however, when a single layer is defined and plasticity is present, the number of integration points is changed to a minimum of five during solution.
The following additional capabilities are available when defining shell layers:
SHELL281 accepts the preintegrated shell section type (SECTYPE,,GENS).
When the element is associated with the GENS section type, thickness or material definitions are not required.
You can use the function tool to define thickness as a function of global/local coordinates or node numbers (SECFUNCTION).
You can specify offsets (SECOFFSET).
The layers are stacked from the shell bottom surface in the direction of shell normal N, which is aligned with the third element coordinate axis e3. The definition of e3 is described below.
Element and Layer Coordinate Systems
SHELL281 has element coordinate systems (e1-e2-e3) established at four in-plane integration points:
When KEYOPT(11) = 0, the default first element coordinate axis e1 is aligned with the first parametric direction S1 of the element at the in-plane integration points. S1 and the second parametric direction S2 can be defined respectively as:
where the geometry is given as:
where: |
= two isoparametric element coordinates |
= shape functions associated with eight element nodes |
= global nodal coordinates of the eight element nodes |
With KEYOPT(11) = 1, the default first element coordinate axis e1 is directed from node I to node J.
The default third element coordinate axis e3 is normal to the element surface, and the default second element coordinate axis e2 is perpendicular to the e1 and e3 axes. Coordinate axes e3 and e2 are obtained respectively as follows:
As shown in the following figure, you can also define element orientation via ESYS. The user-defined element coordinate system (e1-e2-e3) is obtained by projecting a local coordinate system (x-y-z) to the shell surface. When KEYOPT(4) = 0, the user-defined third element coordinate axis e3 is always aligned with the default e3. When KEYOPT(4) = 1, the user-defined e3 is set to the opposite of default e3 if local coordinate axis z and default e3 are in the opposite directions.
The layer coordinate systems (L1-L2-L3) as shown in the following figure are identical to the element coordinate system if no layer orientation angles are specified; otherwise, the layer coordinate system can be generated by rotating the element coordinate system about e3. (For the definition of layer orientation angles θ, see SECDATA.) Material properties are defined in the layer systems; therefore, the layer system is also called the material coordinate system.
Other Input
The element supports degeneration into a triangular form. For better accuracy, however, Ansys, Inc. recommends quadrilateral shaped elements. The triangle form is generally more robust when using the membrane option with large deflections.
To evaluate stresses and strains on exterior surfaces, set KEYOPT(1) = 2. When used as overlaid elements on the faces of 3D elements, this option is similar to the surface stress option, but is more general and applicable to nonlinear analysis. The element used with this option provides no stiffness, mass, or load contributions. Use this option in single-layer shells only. Irrespective of other settings, SHELL281 provides stress and strain output at the four in-plane integration points of the layer.
SHELL281 uses a penalty method to relate the independent rotational degrees of freedom about the normal (to the shell surface) with the in-plane components of displacements. The program determines an appropriate penalty stiffness by default. A drill-stiffness factor can be specified via SECCONTROL. Default drill stiffness is calculated from linear section stiffness (integrated linear elastic material stiffness through the thickness). The default drill stiffness remains constant even when materials become nonlinear. For elements with softening materials, a smaller drill-stiffness scaling factor should be specified via SECCONTROL.
Element loads are described in Element Loading. Pressures may be input as surface loads on the element faces as shown by the circled numbers in Figure 281.1: SHELL281 Geometry. Positive pressures act into the element. Because shell edge pressures are input on a per-unit-length basis, per-unit-area quantities must be multiplied by the shell thickness.
Temperatures may be input as element body loads at the corners of the outside faces of the element and at the corners of the interfaces between layers. The first corner temperature T1 defaults to TUNIF. If all other temperatures are unspecified, they default to T1. If KEYOPT(1) = 0 and if exactly NL+1 temperatures are input, one temperature is used for the four bottom corners of each layer, and the last temperature is used for the four top corner temperatures of the top layer. If KEYOPT(1) = 1 and if exactly NL temperatures are input, one temperature is used for the four corners of each layer. That is, T1 is used for T1, T2, T3, and T4; T2 (as input) is used for T5, T6, T7, and T8, etc. For any other input pattern, unspecified temperatures default to TUNIF.
SHELL281 includes the effects of transverse shear deformation. The transverse shear stiffness of the element is a 2x2 matrix as shown below:
To define transverse shear stiffness values, issue the SECCONTROL command.
Transverse shear-correction factors k are calculated once at the start of the analysis for each section. The material properties used to evaluate the transverse shear correction factors are at the current reference temperature during solution. User-field variables and frequency are all set to zero when evaluating the material properties used to calculate the transverse shear correction factors.
where shear-correction factor k = 5/6, G = shear modulus, and h = thickness of the shell.
The bending stiffness is defined by either a standard or preintegrated shell section (SECTYPE,,SHELL or GENS, respectively).
Further bending-stiffness scaling is available via a user-specified factor
(BENSTIF
on the SECCONTROL command). For a
standard shell section, Mechanical APDL rebalances the element stresses to reflect the change in bending
stiffness.
SHELL281 can be associated with linear elastic, elastoplastic, creep, or hyperelastic material properties. Only isotropic, anisotropic, and orthotropic linear elastic properties can be input for elasticity. The von Mises isotropic hardening plasticity models can be invoked with BISO (bilinear isotropic hardening) and NLISO (nonlinear isotropic hardening) options. The kinematic hardening plasticity models can be invoked with BKIN (bilinear kinematic hardening) and CHABOCHE (nonlinear kinematic hardening). Invoking plasticity assumes that the elastic properties are isotropic (that is, if orthotropic elasticity is used with plasticity, the program assumes the isotropic elastic modulus = EX and Poisson's ratio = NUXY).
Hyperelastic material properties (2, 3, 5, or 9 parameter Mooney-Rivlin material model, Neo-Hookean model, polynomial form model, Arruda-Boyce model, and user-defined model) can be used with this element. Poisson's ratio is used to specify the compressibility of the material. If less than 0, Poisson's ratio is set to 0; if greater than or equal to 0.5, Poisson's ratio is set to 0.5 (fully incompressible).
Both isotropic and orthotropic thermal expansion coefficients can be input using MP,ALPX. When used with hyperelasticity, isotropic expansion is assumed.
Use the TREF command to specify the global value of reference temperature. If MP,REFT is defined for the material number of the element, it is used for the element instead of the value from the TREF command. But if MP,REFT is defined for the material number of the layer, it is used instead of either the global or element value.
When KEYOPT(5) = 0, SHELL281 uses an advanced shell formulation that accurately incorporates initial curvature effects. The calculation for effective shell-curvature change accounts for both shell-membrane and thickness strains. The new formulation generally offers improved accuracy in curved-shell structure simulations, especially when thickness strain is significant or the material anisotropy in the thickness direction cannot be ignored, or in thick shell structures with unbalanced laminate construction or shell offsets..
When KEYOPT(5) = 1, a simplified curved-shell formulation is adopted. Unlike the advanced curved-shell formulation (KEYOPT(5) = 0), the curvature effects in the shell-offset handling are ignored. The simplified formulation generally leads to more robust nonlinear convergence.
The curved-shell formulation is automatically disabled for excessively thick and curved structures with an r / t ratio below 5 / 6, where r is the radius of curvature measured at shell mid-plane and t is the total shell thickness.
KEYOPT(8) = 2 stores midsurface results in the results file for single or multi-layer shell elements. If you use SHELL,MID, you will see these calculated values, rather than the average of the TOP and BOTTOM results. Use this option to access these correct midsurface results (membrane results) for those analyses where averaging TOP and BOTTOM results is inappropriate; examples include midsurface stresses and strains with nonlinear material behavior, and midsurface results after mode combinations that involve squaring operations such as in spectrum analyses.
KEYOPT(9) = 1 reads initial thickness data from a user subroutine.
KEYOPT(10) = 1 outputs normal stress component Sz, where z is shell
normal direction. The element uses a plane-stress formulation that always leads to zero thickness
normal stress. With KEYOPT(10) = 1, Sz is independently recovered during the element solution
output from the applied pressure load. The pressure must be applied directly to the shell, and
not via surface elements (SURFnnn
).
The effects of pressure load stiffness are automatically included for this element. If an unsymmetric matrix is needed for pressure load stiffness effects, use NROPT,UNSYM.
The element supports both consistent and lumped mass matrices. Use LUMPM,ON to activate a lumped mass matrix. A consistent mass matrix is used by default.
A summary of the element input is given in "SHELL281 Input Summary". A general description of element input is given in Element Input.
SHELL281 Input Summary
- Nodes
I, J, K, L, M, N, O, P
- Degrees of Freedom
UX, UY, UZ, ROTX, ROTY, ROTZ if KEYOPT(1) = 0
UX, UY, UZ if KEYOPT(1) = 1
- Material Properties
TB command: See Element Support for Material Models for this element. MP command: EX, EY, EZ, (PRXY, PRYZ, PRXZ, or NUXY, NUYZ, NUXZ), ALPX, ALPY, ALPZ (or CTEX, CTEY, CTEZ or THSX, THSY, THSZ), DENS, GXY, GYZ, GXZ, ALPD Specify BETD, ALPD, DMPR, or DMPS for the element (all layers) by issuing the MAT command to assign the material property set. REFT may be specified once for the element, or may be assigned on a per-layer basis. See the discussion in "SHELL281 Input Summary" for more information. - Surface Loads
- Body Loads
- Temperatures --
For KEYOPT(1) = 0 (Bending and membrane stiffness):
T1, T2, T3, T4 (at bottom of layer 1), T5, T6, T7, T8 (between layers 1-2); similarly for between next layers, ending with temperatures at top of layer NL(4*(NL+1) maximum). Hence, for one-layer elements, eight temperatures are used.
For KEYOPT(1) = 1 (Membrane stiffness only):
T1, T2, T3, T4 for layer 1, T5, T6, T7, T8 for layer 2, similarly for all layers (4*NL maximum). Hence, for one-layer elements, four temperatures are used.
- Special Features
Birth and death Coriolis effect Element technology autoselect Initial state Large deflection Large strain Linear perturbation Nonlinear stabilization Section definition for layered shells and preintegrated general shell sections for input of homogeneous section stiffnesses - KEYOPT(1)
Element stiffness:
- 0 --
Bending and membrane stiffness (default)
- 1 --
Membrane stiffness only
- 2 --
Stress/strain evaluation only
- KEYOPT(4)
Shell normal orientation option:
- 0 --
Calculated from element connectivity (default)
- 1 --
Controlled by the z coordinate direction of a local coordinate system
- KEYOPT(5)
Curved-shell formulation:
- 0 --
Advanced curved shell formation (default)
- 1 --
Simplified curved shell formation
- KEYOPT(8)
Specify layer data storage:
- 0 --
For multi-layer elements, store data for bottom of bottom layer and top of top layer. For single-layer elements, store data for TOP and BOTTOM. (Default)
- 1 --
Store data for TOP and BOTTOM, for all layers (multi-layer elements). (The volume of data may be considerable.)
- 2 --
Store data for TOP, BOTTOM, and MID for all layers; applies to single- and multi-layer elements
- KEYOPT(9)
User thickness option:
- 0 --
No user subroutine to provide initial thickness (default)
- 1 --
Read initial thickness data from user subroutine
UTHICK
For more information, see Subroutine uthick (Getting User-Defined Initial Thickness) in the Programmer's Reference.
- KEYOPT(10)
Thickness normal stress (Sz) output option:
- 0 --
Sz not modified (default, Sz = 0)
- 1 --
Recover and output Sz from applied pressure load
- KEYOPT(11)
Default element x axis (x0) orientation:
- 0 --
First parametric direction at the four in-plane integration points (default)
- 1 --
Pointing from element node I to element Node J
SHELL281 Output Data
The solution output associated with the element is in two forms:
Nodal displacements included in the overall nodal solution
Additional element output as shown in Table 281.1: SHELL281 Element Output Definitions
Several items are illustrated in Figure 281.5: SHELL281 Stress Output.
KEYOPT(8) controls the amount of data output to the results file for processing with the LAYER command. Interlaminar shear stress is available as SYZ and SXZ evaluated at the layer interfaces. KEYOPT(8) must be set to either 1 or 2 to output these stresses in the POST1 postprocessor. A general description of solution output is given in Solution Output. See the Basic Analysis Guide for ways to review results.
The element stress resultants (N11, M11, Q13, etc.) are parallel to the element coordinate system, as are the membrane strains and curvatures of the element. Such generalized strains are available through the SMISC option at the element centroid only. The transverse shear forces Q13, Q23 are available only in resultant form: that is, use SMISC,7 (or 8). Likewise, the transverse shear strains, γ13 and γ23, are constant through the thickness and are only available as SMISC items (SMISC,15 and SMISC,16, respectively).
The program calculates moments (M11, M22, M12) with respect to the shell reference plane. By default, the program adopts the shell midplane as the reference plane. To offset the reference plane to any other specified location, issue the SECOFFSET command. When there is a nonzero offset (L) from the reference plane to the midplane, moments with respect to the midplane () can be recovered from stress resultants with respect to the reference plane as follows:
SHELL281 does not support extensive basic element printout. POST1 provides more comprehensive output processing tools; therefore, it is good practice to issue the OUTRES command to ensure that the required results are stored in the database.
SHELL281 allows for transformation of stresses and strains to other coordinate systems in postprocessing (RSYS). By default, the element stresses and strains are displayed or listed in the global Cartesian coordinate system.
Figure 281.5: SHELL281 Stress Output
x0 = Element x axis if element orientation (ESYS) is not specified. (See KEYOPT(11).) x = Element x axis if element orientation is specified.
The Element Output Definitions table uses the following notation:
A colon (:) in the Name column indicates that the item can be accessed by the Component Name method (ETABLE, ESOL). The O column indicates the availability of the items in the file jobname.out. The R column indicates the availability of the items in the results file.
In either the O or R columns, “Y” indicates that the item is always available, a letter or number refers to a table footnote that describes when the item is conditionally available, and “-” indicates that the item is not available.
Table 281.1: SHELL281 Element Output Definitions
Name | Definition | O | R |
---|---|---|---|
EL | Element number and name | Y | Y |
NODES | Nodes - I, J, K, L | - | Y |
MAT | Material number | - | Y |
THICK | Average thickness | - | Y |
VOLU: | Volume | - | Y |
XC, YC, ZC | Location where results are reported | - | 4 |
PRES | Pressures P1 at nodes I, J, K, L; P2 at I, J, K, L; P3 at J,I; P4 at K,J; P5 at L,K; P6 at I,L | - | Y |
TEMP | T1, T2, T3, T4 at bottom of layer 1, T5, T6, T7, T8 between layers 1-2, similarly for between next layers, ending with temperatures at top of layer NL(4*(NL+1) maximum) | - | Y |
LOC | TOP, MID, BOT, or integration point location | - | 1 |
S:X, Y, Z, XY, YZ, XZ | Stresses | 3 | 1 |
S:1, 2, 3 | Principal stresses | - | 1 |
S:INT | Stress intensity | - | 1 |
S:EQV | Equivalent stress | - | 1 |
EPEL:X, Y, Z, XY | Elastic strains | 3 | 1 |
EPEL:EQV | Equivalent elastic strains [7] | - | 1 |
EPTH:X, Y, Z, XY | Thermal strains | 3 | 1 |
EPTH:EQV | Equivalent thermal strains [7] | - | 1 |
EPPL:X, Y, Z, XY | Average plastic strains | 3 | 2 |
EPPL:EQV | Equivalent plastic strains [7] | - | 2 |
EPCR:X, Y, Z, XY | Average creep strains | 3 | 2 |
EPCR:EQV | Equivalent creep strains [7] | - | 2 |
EPTO:X, Y, Z, XY | Total mechanical strains (EPEL + EPPL + EPCR) | 3 | - |
EPTO:EQV | Total equivalent mechanical strains (EPEL + EPPL + EPCR) | - | - |
NL:SEPL | Plastic yield stress | - | 2 |
NL:EPEQ | Accumulated equivalent plastic strain | - | 2 |
NL:CREQ | Accumulated equivalent creep strain | - | 2 |
NL:SRAT | Plastic yielding (1 = actively yielding, 0 = not yielding) | - | 2 |
NL:PLWK | Plastic work/volume | - | 2 |
NL:HPRES | Hydrostatic pressure | - | 2 |
SEND:ELASTIC, PLASTIC, CREEP, ENTO | Strain energy densities | - | 2 |
N11, N22, N12 | In-plane forces (per unit length) | - | Y |
M11, M22, M12 | Out-of-plane moments (per unit length) | - | 8 |
Q13, Q23 | Transverse shear forces (per unit length) | - | 8 |
ε11, ε22, ε12 | Membrane strains | - | Y |
k11, k22, k12 | Curvatures | - | 8 |
γ13, γ23 | Transverse shear strains | - | 8 |
LOCI:X, Y, Z | Integration point locations | - | 5 |
SVAR:1, 2, ... , N | State variables | - | 6 |
ILSXZ | SXZ interlaminar shear stress | - | Y |
ILSYZ | SYZ interlaminar shear stress | - | Y |
ILSUM | Magnitude of the interlaminar shear stress vector | - | Y |
ILANG | Angle of interlaminar shear stress vector (measured from the element x axis toward the element y axis in degrees) | - | Y |
Sm: 11, 22, 12 | Membrane stresses | - | Y |
Sb: 11, 22, 12 | Bending stresses | - | Y |
Sp: 11, 22, 12 | Peak stresses | - | Y |
St: 13, 23 | Averaged transverse shear stresses | - | Y |
The following stress solution repeats for top, middle, and bottom surfaces.
Nonlinear solution output for top, middle, and bottom surfaces, if the element has a nonlinear material, or if large-deflection effects are enabled (NLGEOM,ON) for SEND.
Stresses, total strains, plastic strains, elastic strains, creep strains, and thermal strains in the element coordinate system are available for output (at all section points through thickness). If layers are in use, the results are in the layer coordinate system.
Available only at centroid as a *GET item.
Available only if OUTRES,LOCI is used.
Available only if the UserMat subroutine and TB,STATE command are used.
The equivalent strains use an effective Poisson's ratio: for elastic and thermal this value is set by the user (MP,PRXY); for plastic and creep this value is set at 0.5.
Not available for KEYOPT(1) = 1 (membrane only) or KEYOPT(1) = 2 (stress/strain evaluation only).
Table 281.2: SHELL281 Item and Sequence Numbers lists output available through ETABLE using the Sequence Number method. See Creating an Element Table and The Item and Sequence Number Table for more information. The following notation is used in Table 281.2: SHELL281 Item and Sequence Numbers:
- Name
output quantity as defined in the Table 281.1: SHELL281 Element Output Definitions
- Item
predetermined
Item
label for ETABLE- E
sequence number for single-valued or constant element data
- I,J,K,L
sequence number for data at nodes I, J, K, L
Table 281.2: SHELL281 Item and Sequence Numbers
Output Quantity Name | ETABLE and ESOL Command Input | |||||
---|---|---|---|---|---|---|
Item | E | I | J | K | L | |
N11 | SMISC | 1 | - | - | - | - |
N22 | SMISC | 2 | - | - | - | - |
N12 | SMISC | 3 | - | - | - | - |
M11 | SMISC | 4 | - | - | - | - |
M22 | SMISC | 5 | - | - | - | - |
M12 | SMISC | 6 | - | - | - | - |
Q13 | SMISC | 7 | - | - | - | - |
Q23 | SMISC | 8 | - | - | - | - |
ε11 | SMISC | 9 | - | - | - | - |
ε22 | SMISC | 10 | - | - | - | - |
ε12 | SMISC | 11 | - | - | - | - |
k11 | SMISC | 12 | - | - | - | - |
k22 | SMISC | 13 | - | - | - | - |
k12 | SMISC | 14 | - | - | - | - |
γ13 | SMISC | 15 | - | - | - | - |
γ23 | SMISC | 16 | - | - | - | - |
P1 | SMISC | - | 18 | 19 | 20 | 21 |
P2 | SMISC | - | 22 | 23 | 24 | 25 |
P3 | SMISC | - | 27 | 26 | - | - |
P4 | SMISC | - | - | 29 | 28 | - |
P5 | SMISC | - | - | - | 31 | 30 |
P6 | SMISC | - | 32 | - | - | 33 |
P1 | SMISC | - | 18 | 19 | 20 | 21 |
P2 | SMISC | - | 22 | 23 | 24 | 25 |
P3 | SMISC | - | 27 | 26 | - | - |
P4 | SMISC | - | - | 29 | 28 | - |
P5 | SMISC | - | - | - | 31 | 30 |
P6 | SMISC | - | 32 | - | - | 33 |
Sm: 11 | SMISC | 34 | - | - | - | - |
Sm: 22 | SMISC | 35 | - | - | - | - |
Sm: 12 | SMISC | 36 | - | - | - | - |
Sb: 11 | SMISC | 37 | - | - | - | - |
Sb: 22 | SMISC | 38 | - | - | - | - |
Sb: 12 | SMISC | 39 | - | - | - | - |
Sp: 11 (at shell bottom) | SMISC | 40 | - | - | - | - |
Sp: 22 (at shell bottom) | SMISC | 41 | - | - | - | - |
Sp: 12 (at shell bottom) | SMISC | 42 | - | - | - | - |
Sp: 11 (at shell top) | SMISC | 43 | - | - | - | - |
Sp: 22 (at shell top) | SMISC | 44 | - | - | - | - |
Sp: 12 (at shell top) | SMISC | 45 | - | - | - | - |
St: 13 | SMISC | 46 | - | - | - | - |
St: 23 | SMISC | 47 | - | - | - | - |
THICK | NMISC | 1 | - | - | - | - |
Output Quantity Name | ETABLE and ESOL Command Input | ||||
Item | Bottom of Layer i | Top of Layer i | |||
ILSXZ | SMISC | 8 * (i - 1) + 51 | 8 * (i - 1) + 52 | ||
ILSYZ | SMISC | 8 * (i - 1) + 53 | 8 * (i - 1) + 54 | ||
ILSUM | SMISC | 8 * (i - 1) + 55 | 8 * (i - 1) + 56 | ||
ILANG | SMISC | 8 * (i - 1) + 57 | 8 * (i - 1) + 58 |
SHELL281 Assumptions and Restrictions
Zero-area elements are not allowed. (Zero-area elements occur most often whenever the elements are numbered improperly.)
Zero-thickness elements or elements tapering down to a zero thickness at any corner are not allowed (but zero-thickness layers are allowed).
The total thickness of each SHELL281 element should be less than twice that of the curvature radius.
Use at least two elements in each direction to avoid hourglass mode.
If multiple load steps are used, the number of layers cannot change between load steps.
When the element is associated with preintegrated shell sections (SECTYPE,,GENS), additional restrictions apply. For more information, see Considerations for Using Preintegrated Shell Sections in the Structural Analysis Guide.
No slippage is assumed between the element layers. Shear deflections are included in the element; however, normals to the center plane before deformation are assumed to remain straight after deformation.
Transverse shear stiffness of the shell section is estimated by an energy equivalence procedure (of the generalized section forces and strains vs. the material point stresses and strains). The accuracy of this calculation may be adversely affected if the ratio of material stiffnesses (Young's moduli) between adjacent layers is very high.
The calculation of interlaminar shear stresses is based on simplifying assumptions of unidirectional, uncoupled bending in each direction. If accurate edge interlaminar shear stresses are required, shell-to-solid submodeling should be used.
The section definition permits use of hyperelastic material models and elastoplastic material models in laminate definition. However, the accuracy of the solution is primarily governed by fundamental assumptions of shell theory. The applicability of shell theory in such cases is best understood by using a comparable solid model.
The layer orientation angle has no effect if the material of the layer is hyperelastic.
The through-thickness stress, SZ, is always zero.
This element works best with full Newton-Raphson solution scheme (NROPT,FULL,,ON).
Stress stiffening is always included in geometrically nonlinear analyses (NLGEOM,ON). Prestress effects can be activated via the PSTRES command.
In a nonlinear analysis, the solution process terminates if the thickness at any integration point that was defined with a nonzero thickness vanishes (within a small numerical tolerance).
If a shell section has only one layer and the number of section integration points is equal to one, or if KEYOPT(1) = 1, then the shell has no bending stiffness, a condition that can result in solver and convergence problems.
SHELL281 Product Restrictions
When used in the product(s) listed below, the stated product-specific restrictions apply to this element in addition to the general assumptions and restrictions given in the previous section.
Ansys Mechanical Pro —
Birth and death is not available.
Initial state is not available.
Section definition for layered shells is not available.