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Customer Training Material
Appendix 2A
Element Technology
Structural Nonlinearities
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ANSYS Mechanical Element Technology
Customer Training MaterialOverview
This is an optional lecture intended for users who want to obtain a
better understanding of element technology options used in
s ruc ura non near s mu a ons.
With the variety of technologies available in many elements,
choosing the best element formulation option to solve problems
most efficiently can be challenging.
Fortunately, WB Mechanical will automatically activate the best
options based on the analysis challenges present in the model.
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ANSYS Mechanical Element Technology
Customer Training Material Overview
However, the analyst of nonlinear problems still has decisions to
make. For example, since large nonlinear models can be very
c a eng ng an compu a ona y expens ve, s some mes
advantageous to drop element mid-side nodes.
Advantages to lower order elements:
Runtime Efficiency
Computational Stability
Disadvantage to lower order elements:
Shear Locking with conventional,
displacement based formulations in
en ng om na e pro ems. To address this challenge, WB-
Mechanical automatically enhances the
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technology.
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Customer Training Material Overview
In addition, material incompressibility can also present problems with
conventional formulations. In anticipation of this challenge, WB-
.
Solution output reports when Mixed u-P is activated.
Solution out ut also re orts its effects on conver ence
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ANSYS Mechanical Element Technology
Customer Training Material Overview
The general recommendation is to accept the automatic formulation
settings when they are activated.
It is however im ortant to understand them:
What triggers these changes to element formulation? What are the effects on convergence patterns and results?
With these questions in mind, the following topics will be covered:
A. Conventional Displacement Formulation.
C. Selective Reduced Integration (B-bar)
D. Uniform Reduced Integration (URI)
. F. Simplified Enhanced Strain (SES)
G. Mixed u-P Formulation
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ANSYS Mechanical Element Technology
Customer Training MaterialA. Conventional Displ. Formulation
For any element, DOF solution uis solved at nodes
Stresses and strains are calculated at
inte ration oints. The are derived from
DOF. For example, we can determine
strains from displacements via:,
uB =
Where B is called the strain-displacement matrixu
en we pos -process resu s, s ress s ra n va ues a
integration points are extrapolated or copied to nodal
locations
The image on the right shows a 4-node quad element
with 2x2 integration, integration points shown in red.
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ANSYS Mechanical Element Technology
Customer Training Material Conventional Displ. Formulation
Integration points for conventional displacement-based elements
follow Gauss quadrature rules and are the same order as the element.
This is called full integration.
Element Type Full Integration Order
8 Node Quad 3x3
8 Node Hex 2x2x2
20 Node Hex 3x3x31
In other words, full integration means that the numerical integration
rule is accurate for all components of strain energy for geometrically
.
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1 Note that ANSYS uses a 14pt integration scheme, which is also considered full
integration
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ANSYS Mechanical Element Technology
Customer Training Material... Conventional Displ. Formulation
Fully integrated, lower-order conventional displacement elements are
susceptible to shear and volumetric locking, so they are rarely, if
ever, used.
Fully integrated, higher-order conventional displacement elementsare also prone to volumetric locking.
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ANSYS Mechanical Element Technology
Customer Training MaterialB. Shear and Volumetric Locking
There are two problems with conventional displacement-based
elements: shear locking and volumetric locking:
Shear Lockingresults in bending behavior being too stiff(parasitic
shear stresses). This is a property of the geometry, when thinmembers are subject to bending.
Volumetric Lockingresults in overly stiffresponse. This is a
property of the material, when the Poissons ratio is near or equal
to 0.5.
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ANSYS Mechanical Element Technology
Customer Training Material... Shear Locking
Fully integrated lower order elements exhibit overstiffness in
bending problems. This formulation includes shear strains in
, .
Below are element shear strain plots in MAPDL. Both beams are identicalin geometry, material properties, boundary conditions and loading.
Higher Order Elements
produce correct results
Lower Order Elements with
conventional, fully integrated,
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bending produces shear locking
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ANSYS Mechanical Element Technology
Customer Training Material... Shear Locking
Recall, for a beam in pure bending the shear strain is zero.
y
M M x
Correct Response:
Pure bending deformation for
a differential volume, plane
Shear Locking:
Fully integrated lower order
element deformation, top and
sections remain plane, topand bottom edges become
arcs, xy = 0.bottom edges remain straight,right angles are not preserved,xy is non zero.
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ANSYS Mechanical Element Technology
Customer Training Material... Volumetric Locking
Volumetric locking occurs in fully integrated elements when the
material behavior is nearly or fully incompressible (Poissons ratio
approaches or equals 0.5).
The incompressibility can occur from a hyperelastic material or plasticflow (discussed later).
,
element to have an overstiffness for deformations that should not
cause any volume change.
.
Volumetric locking can occur for various stress states, including
plane strain, axisymmetric, and 3-D stress.
For plane stress problems, volumetric locking does not occur becauseout-of-plane strains are used to satisfy incompressibility condition.
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ANSYS Mechanical Element Technology
Customer Training Material... Example of Volumetric Locking
Contours of hydrostatic pressure results in conventional elements
are shown below (ANSYS Results Plot (NL,HPRES)).
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ANSYS Mechanical Element Technology
Customer Training Material... Volumetric Locking
We can separate stress into volumetric (-p) and deviatoric (s)components:
sI += p
p -p
3 p 3 -
= +
Stress State
(Where: = 2 = 3) Hydrostatic stress (p) causingvolume change only Deviatoric stress (s) causingangular distortion only2 3 2 -p 3
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ANSYS Mechanical Element Technology
Customer Training Material... Volumetric Locking
The hydrostatic pressure (p) is defined as the product of the bulkmodulus (K) and volumetric strain (vol):
volKp =
zyx ++=3
( )K
=
213
( )zyxvol
++=
21
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zyxE
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Customer Training Material... Volumetric Locking
From the equations on the previous slide, if Poissons ratio is near
or equal to 0.5, we can see that:
Volumetric strain volwill be near or equal to zero This is called nearlyor fully incompressible material behavior
Nearly or fully incompressible materials present numerical
difficulties, and they also exhibit overly stiff behavior.
From a computational standpoint, nearly incompressible and fully
incompressible problems are treated differently.
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ANSYS Mechanical Element Technology
Customer Training Material... Example of Volumetric Locking
Example of Volumetric Locking in Thick-Walled Cylinder with
Conventional displacement based elements
As incompressibility,
locking develops,
resulting in unacceptable
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%18 Error in
displacement calculation
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ANSYS Mechanical Element Technology
Customer Training Material... Element Control
The 18x series of structural elements that WB-Mechanical usesoffers up to five different technologies to address potentialproblems with shear and volumetric locking: B-Bar, URI, ES, SES,
.
ogy
rder
s rder
s cking
) essible
ty,sticity)
essible
asticity)
Element
Technol
Lower-O
Element
Higher-
Element
ShearL
(Bendin
Nearly-
Incompr
(Plastici
Hyperel
Fully-
Incompr
(Hyperel
B-Bar Y - N Y N
Enhanced Strain Y - Y Y NSim lified Enhanced Strain Y - Y N N
Higher-order 18x elements (PLANE183, SOLID186-187) use URI by default.
URI Y Y Y Y N
Mixed U-P Y Y N Y Y
.
Lower-order 18x elements (PLANE182, SOLID185) use ES by default, except whenhyperelastic material is assigned..
B-Bar, ES, and SES are not applicable to higher-order elements.
Mixed u-P technolo is inde endent of the others so ma or ma not be activated
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in conjunction with B-Bar or URI.
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ANSYS Mechanical Element Technology
Customer Training Material Element Control
The element technology is defined by a particular key option
(KEYOPT):
KEYOPTS are switches, used to turn various element options on or off.
KEYOPTS have many applications. Controlling element technology is just
one use.
For example, PLANE182 element uses KEYOPT(1) to define which
ec no ogy s use an o con ro m xe u- ormu a on
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Refer to the Elements Reference Manual for more details on each of the
18x element types and their respective key options.
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Customer Training Material Element Control
The syntax for the KEYOPT command is as follows:
KEYOPT, ITYPE, KNUM, VALUE
Where ITYPEis the Element t e number
KNUMis the number of the KEYOPT
VALUEis the value of this KEYOPT
Example, if element type#1 is PLANE182, enhanced strain can beactivated with the following command:
KEYOPT 1 1 2
Key Option Number (for element technology)
Key Option Value (for enhanced strain)
Element Type Number
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Refer to the ANSYS Commands Manual for more details
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ANSYS Mechanical Element Technology
Customer Training MaterialFormulations
The next few sections present details on each of the formulations
used in WB-Mechanical 18X Structural elements
C. Selective Reduced Integration (B-bar)D. Uniform Reduced Integration (URI)
.
F. Simplified Enhanced Strain (SES)
G. Mixed u-P Formulation
-.
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ANSYS Mechanical Element Technology
Customer Training MaterialC. The B-Bar Method
The B-bar method (a.k.a., selective reduced integration, constant
dilatational elements, constant pressure approach) uses an
.
Recall that the stress state can be separated in hydrostatic (p) anddeviatoric (s) terms.
sI
K
p
=
+=
es G
vo
2
=
=
In the above equation, vol is volumetric strain and e is deviatoric strain.
Kis the bulk modulus and Gis the shear modulus.
vo
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ANSYS Mechanical Element Technology
Customer Training Material... The B-Bar Method
Strains are related to displacements via the following:
BBBdv
+=
B
B v
v= VdV
uB
BBBdv
=
+=
When evaluating B, however, we will use two different integration
orders for volumetric and deviatoric components.
Bv is evaluated with one integration point(reduced integration)
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On the other hand, Bd is evaluated with 2x2
integration points (full integration)
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ANSYS Mechanical Element Technology
Customer Training Material... The B-Bar Method
As shown on the previous slide, the volumetric and deviatoric
components of B are not evaluated at the same order of integration.
Only the volumetric component Bvhas reduced integration. That is
why this method is called selective reduced integration or constant
pressure approach. It is also known as the B-bar methodbecause Bis averaged on the volumetric term.
uB = The fact that the volumetric term Bvhas reduced integration allows it
to be softer since it is not fully integrated. This allows for solution
of nearly incompressible behavior and overcomes volumetric
oc ng. However, because the deviatoric term Bdremains the same, parasitic
shear strains still exist, so this formulation is still susceptible to
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shear locking.
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ANSYS Mechanical Element Technology
Customer Training MaterialD. Uniform Reduced Integration
Uniform Reduced Integration (URI) uses an integration rule one orderlower than needed for numerically exact integration
Element Type Ful l Integration
Order1
Reduced Integration
Order4 Node Quad 2x2 1x1
8 Node Hex 2x2x2 1x1x1
20 Node Hex 3x3x3 2x2x2
,and deviatoric terms have reduced integration.
This formulation leads to a more element flexibility which helpseliminate shear and volumetric locking.
Reduced integration of volumetric terms allows solution of nearlyincompressible problems.
Reduced integration of deviatoric terms prevents shear locking in bending
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1 This is full integration as noted in literature, not necessarily related to 18x elements implementation
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ANSYS Mechanical Element Technology
Customer Training Material... Uniform Reduced Integration
Unfortunately, the reduced integration of deviatoric terms causes
modes of deformation which have zero strain energy, called zero
modes of deformation which lead to physically unrealistic behavior.
In the lower order element with one integration point shown below,
point does not capture any strain energy in the element.
By default, Mechanical, will not use the URI option in the lower order
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PLANE182 and SOLID185 elements.
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ANSYS Mechanical Element Technology
Customer Training Material... Uniform Reduced Integration
URI elements have many nice benefits:
Can be used in nearly incompressible problems to overcome volumetric
lockin
Can be used in bending problems without worrying about shear locking No additional DOF are required, and, in fact, less CPU time is required for
e emen ca cu a ons. e s zes e.g., .esav are re uce . s prov es
efficient solutions, especially for nonlinear problems.
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Customer Training Material... Uniform Reduced Integration
On the other hand, a user needs to consider a few things when using
URI:
Lower-order URI elements are susceptible to hourglassing, hence URI is
not the set automatically by Simulation.
Lower-order URI elements may be too flexible, especially in bending-
dominated problems, so a iner mesh may be required such that
displacements are not over-predicted
Both lower- and higher-order URI elements have an integration rulew c s one or er ower t an u ntegrat on. s means stresses are
evaluated at 1 point for lower-order elements and 2x2 or 2x2x2 for
higher-order elements. Hence, more elements may be required to
ca ture stress radients.
URI cannot be used alone in fully incompressible analyses. For fully-
incompressible situation, URI can be used with Mixed u-P (discussed
later
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ANSYS Mechanical Element Technology
Customer Training MaterialE. Enhanced Strain Formulation
Enhanced Strain Formulation (a.k.a. Incompatible Modes, Assumed
Strain) adds internal degrees of freedom to lower-order quad/hex
elements. The displacement gradient tensor is modified with these
extra enhanced terms, hence the name Enhanced Strain.
Enhanced Strain elements are useful when shear or volumetric locking
are encountered (e.g., bending dominated problems or nearly
incompressible material behavior).
,
quad or hex shape:
PLANE182 when KEYOPT(1)=2
SOLID185 when KEYOPT(2)=2
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Customer Training Material... Enhanced Strain Formulation
This formulation is only applicable for lower-order elements in
quad or hex shape.
emen per orms es w en near y rec angu ar; on e o er an ,
they do not perform well when trapezoidal. This is a limitation of theEnhanced Strain technology.
- .
Shape PLANE182 PLANE183 SOLID185 SOLID187 SOLID186
Rectangular 1.004 1.001 1.005 1.000 1.002
Axial Mode: 1st Natural Frequency Ratio
rapezo . . . . .
Trapezoid (30) 1.004 1.001 1.005 1.000 1.002
Trapezoid (45) 1.005 1.001 1.006 1.000 1.002
Parallelogram (15) 1.004 1.001 1.005 1.000 1.002
Parallelogram (30) 1.004 1.001 1.005 1.000 1.002
Parallelogram (45) 1.004 1.001 1.005 1.000 1.002
Bending Mode: 1st Natural Frequency Ratio
Shape PLANE182 PLANE183 SOLID185 SOLID187 SOLID186
Rectangular 1.010 0.999 1.010 1.004 0.999
Trapezoid (15) 1.567 1.000 1.596 1.005 1.000
Trapezoid (30) 1.973 1.003 2.009 1.008 1.003
Trapezoid (45) 2.207 1.012 2.245 1.020 1.012
Parallelogram (15) 1.040 0.999 1.042 1.005 0.999
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. . . . .
Parallelogram (45) 1.119 0.999 1.126 1.020 0.999
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ANSYS Mechanical Element Technology
Customer Training Material... Enhanced Strain Formulation
Example of Volumetric Locking in Thick-Walled Cylinder
Ri=3,Ro=9
SOLID185 with enhanced strain
SOLID45 with extra shape
Pure elastic material (E=1000)
Different Poissons ratios (nu=0.0, 0.25, 0.3, 0.49, 0.499,0.4999)
Linear analysis
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Customer Training Material... Enhanced Strain Formulation
Example of Volumetric Locking in Thick-Walled Cylinder
Results from older Element 45 Results from Element 185
%18 Error in %1.6 Error in
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Customer Training Material... Enhanced Strain Formulation
Enhanced Strain Formulation was designed for bending and nearly
incompressible applications in mind
Enhanced Strain alone cannot be used for full incom ressible anal ses
but it can be used in conjunction with Mixed u-P (discussed later) for
those situations.
It is enerall not recommend for use with Mixed u-P when bulk
compression is the dominant behavior. In this case B-Bar with Mixed u-P
is considered more effective.
computationally expensive
The extra internal DOF mentioned on the previous slides are condensed
,
*.esav file) associated with it.
Quad PLANE182 and hex SOLID185 use Enhanced Strain
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The Enhanced Strain terms will have little benefit in bending if the
element is distorted, especially if trapezoidal.
ANSYS Mechanical Element Technolog
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ANSYS Mechanical Element Technology
Customer Training Material... Enhanced Strain Formulation
Additional notes on Enhanced Strain Formulation:
By default, the Enhanced Strain Formulation is used for quad or hex
sha e onl . In de enerate form, the Enhanced Strain formulation is not
used, and degenerate shape functions are automatically used instead,
which provides greater robustness for nonlinear solutions.
With the ETCONTROL,,OFF command, re ular sha e functions includin
use of Enhanced Strain formulation) can be used in degenerate form,
although this is not recommended.
Despite the above points, in general, degenerate lower-order elementsshould not be used at all except as fillers in unimportant regions since 3-
node triangles and 4-node tetrahedra are constant strain elements.
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Customer Training MaterialF. Simplified Enhanced Strain
Simplified Enhanced Strain (a.k.a. Extra Displacement Shapes,
Bubble Functions) can be thought of as a subset of Enhanced Strain,
discussed earlier.
Simplified Enhanced Strain has additional internal degrees of freedom for
lower-order quad/hex elements to prevent shear locking only. The extrainternal DOF to treat volumetric locking are not present.
Although the internal DOF are meant to augment the shape functions to
provide more flexibility (as discussed in Section E), this also results in
softening of the element, so volumetric locking is also sometimesa ev a e n rec y o some egree.
However, if material incompressibility is a concern, the user should not
use Simplified Enhanced Strain, as it does not address volumetric
oc ng rec y.
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Customer Training Material... Simplified Enhanced Strain
There are two 18x elements which can use Simplified Enhanced
Strain, when in quad or hex form:
PLANE182 when KEYOPT(1)=3
SOLID185 when KEYOPT(2)=3
Similar to Enhanced Strain, Simplified Enhanced Strain terms will havelittle benefit in bending if the element is distorted, especially if
rapezo a .
For 2D elements (PLANE182), 4 internal DOF are added whereas for, n erna are presen . ese n erna are
condensed out at the element level.
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Customer Training Material... Simplified Enhanced Strain
Simplified Enhanced Strain can be used in situations where shear
locking may be present, but volumetric locking is not an issue
It is a subset of Enhanced Strain, so it may be slightly more efficient
in situations where volumetric locking is not a concern
Simplified Enhanced Strain can be used with Mixed u-P formulation
for nearly- or fully-incompressible situations.
In these cases, there will be no difference in the use of Simplified
Enhanced Strain or regular Enhanced Strain in conjunction withMixed u-P
As noted in Section E, Enhanced Strain does not use extra internal
DOF for volumetric terms if used in conjunction with Mixed u-P.
Hence, Enhanced Strain and Simplified Enhanced Strain will be the
same if Mixed u-P formulation is also activated.
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Customer Training MaterialG. Mixed u-P Formulation
Mixed u-P formulation is used to treat volumetric locking by solving
hydrostatic pressure (or volumetric strain) as an additional DOF.
hydrostatic pressure (or volumetric strain) DOF.
There are three different Mixed u-P formulations that can be used for
Nearly-incompressible elasto-plastic materials (Mixed u-P I)
Fully-incompressible hyperelastic materials (Mixed u-P II)
Nearly-incompressible hyperelastic materials (Mixed u-J)
Only Mixed u-P II is activated automatically in WB-Mechanical when
-
plane stress states. This section will focus on Mixed u-P II only.
Users can refer to the ANSYS documentation for more details on the
- -
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.
the nearly incompressible cases as necessary using a command
object.
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Customer Training Material... Mixed u-P Formulation
When Mixed u-P is activated, hydrostatic pressure is treated as an
independent DOF which is solved for. The matrix equation is:
=
00F
Pu
KKK uPuu
Note: Because the material is fully incompressible, [Kpp
]=0,
Because the Lagrange Multipliers (internal DOF P) are kept in the
assembled stiffness matrix, direct solvers mustbe used with this
ormu a on. era ve so vers suc as canno an e e
resulting ill-conditioned matrices.
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Customer Training Material... Mixed u-P Formulation
For hyperelasticity, the volume ratio (J) is defined as:
V=
where V and Vo are the updated and original volumes of the element,
oV
.
To maintain incompressible behavior, a volumetric compatibilityconstraintmust be satisfied
For fully-incompressible hyperelastic materials, no volume change
should occur.
e use o , e vo ume c ange can e quan e
For fully-incompressible case, J should be equal to 1. In other words, the
final and original volumes should be the same (no volume change)
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Customer Training Material... Mixed u-P Formulation
The discussion on the previous slide emphasized the fact that the
volume ratio Jshould be constant (J=1), which is true for fully
incompressible materials:
This leads to the following volumetric compatibility equation:
01 =J
J1Vtol
V
JV
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Customer Training Material... Mixed u-P Formulation
The default value of Vtol is 1e-5. The Solution Information Branch will
record when this condition is not satisified.
If the model fails to converge because the Mixed u-P volumetric
,
this tolerance.
Note: Loosening this tolerance has the effect of allowing some small
a last resort after other solution convergence options (i.e. increasing thenumber of substeps) have been tried.
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Customer Training Material... Volumetric Tolerance
WB-Mechanical users do not have direct access to the tolerance on
volumetric compatibility constraints, but it can be changed via
Command Objects.
Manuall activatin Mixed u-P is necessar in order for
subsequent solc,,,vtol to be accepted
Solution Information Branch will record this change
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Customer Training Material... Considerations for Mixed u-P
For a fully incompressible problem, no unique solution may exist if all
boundary nodes have prescribed displacements. This is due to the
fact that hydrostatic pressure (internal DOF) is independent of
deformation. Hydrostatic pressure needs to be determined by a
force/pressure boundary condition. Without this, the hydrostaticpressure cannot be calculated i.e., there is no unique solution. For
,
applied boundary condition will remedy this situation.
When the number of pressure DOF (Np) is greater than the number of
active (unconstrained) displacement DOF (Nd), this is an over-
constrained model which results in lockin . Ideall the ratio of
Nd/Np should be 2/1 for 2D problems or 3/1 for 3D problems. Over-constrained models can be overcome by mesh refinement, especially
in areas without displacement constraints.
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Customer Training Material... Considerations for Mixed u-P
WB-Mechanical provides an extensive library of element technologyusing Mixed u-P formulation for nearly and fully incompressible
materials.
Mixed u-P, by itself, addresses the issue of volumetric locking
For fully-incompressible hyperelastic materials, WB-Mechanical mustuse
- .
For nearly-incompressible elasto-plastic material, WB-Mechanical will not
turn on mixed u-P automatically.
Mixed u-P Formulation can be combined with B-bar, URI, Enhanced
Strain, or Simplified Enhanced Strain Formulations in nearly
incompressible applications using command objects.
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Customer Training MaterialH. Solid-Shell Formulation
A special Solid-Shell Element is available to model thin to
moderately-thick shells in 3D form.
This is a 3D 8-node hex element with translational DOF
This element has 7 internal DOF, similar to Enhanced Strain but
decoupled in bending direction. Assumed strain method also used for
- .
These 7 internal DOF are condensed out at the element level
This formulation is available in the SOLSH190 element
There are some situations where use of either shell or regular solid
elements may not be desirable (next slide), so the SOLSH190 element
provides a good solution in these cases
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Customer Training Material Solid-Shell Formulation
Considerations for Shells:
Nonlinear MPC required for
connectin shells to solids for lar e-
Considerations for Solids:
The error in the kinematic
approximation with linear 3D solid
deflection analyses
Currently supported by 17x
elements becomes apparent in
bending dominant problems as
thickness decreases
bonded contact
DOF not continuous at interface
Higher-order 3D solid elements
do not have this problem
Treatment of variable thickness is
complicated
,
as Enhanced Strain, are not
sufficient to remedy this numerical
Currently, AI*Environment
5.0/5.1 supports variable
thickness midsurface extraction
when thickness/ length ratio is very
small
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Limited application to thick shells
ANSYS Mechanical Element Technology
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Customer Training Material Solid-Shell Formulation
Although a 8-node hex element, SOLSH190 element coordinate
system not defined solely by ESYS but by nodal connectivity
- .
Use of VEORIENT (prior to meshing) or EORIENT (aftermeshing) is required to redefine z-axis. Element x- and y-
The nodal connectivity shown on the right of I-J-K-L
forms the bottom face.The top face is formed by M-N-O-P.
The element z-axis is then defined as the
normal of the mid lane shown in li ht blue
Prism form of SOLSH190 is stiff in bending,
so it should only be used as filler elements.
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Customer Training Material Solid-Shell Formulation
SOLSH190 has 2x2x2 integration points
Unlike SHELL elements, SZ is not automatically zero.-
SHELL181 has user-defined section integration pointsthrough-plane (section definition) and either 1 or 2x2integration points in-plane. SOLSH190 currently has afixed number of integration points. This is an important
consideration for nonlinear materials since more thanone element through the thickness may be required (seeexample below, 2 elements thru thickness)
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E l f S lid Sh ll El t
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Customer Training Material Example of Solid-Shell Element
Simple example of buckling of arch
shown on right
Comparison of SHELL181,
SOLID185 (Simplified Enhanced
Strain), and SOLSH190 For thin structures, SOLSH190
3rd mode thick
SOLID185 requires additional
elements along edge
For thick structures, SOLSH190
. - . - . - . .
SHELL181 1 10 3.7496 3750 3.74E +06 3.09E+09 1.64E+10
20 3.4509 3451 3.44E +06 2.89E+09 1.57E+10
50 3.3743 3374 3.37E +06 2.84E+09 1.55E+10
SOLID185 1 10 3533.8000 39403 4.31E+06 3.55E+09 2.23E+10
20 50.9320 4096 3.48E +06 3.23E+09 2.07E+10
matches SOLID185. . . .
3 10 3534.0000 39403 4.31E+06 3.49E+09 2.13E+10
20 50.8300 4096 3.48E +06 3.18E+09 1.99E+10
50 3.6230 3386 3.38E+06 3.10E+09 1.96E+10
5 10 3533.8000 39403 4.31E+06 3.45E+09 2.04E+10
20 50.9040 4096 3.48E +06 3.14E+09 1.91E+10
. . . .
SOLSH190 1 10 3.7232 3722 3.72E+06 3.40E+09 2.23E+10
20 3.4530 3445 3.44E+06 3.17E+09 2.07E+10
50 3.3751 3373 3.37E+06 3.11E+09 2.04E+10
3 10 3.6055 3722 3.72E+06 3.37E+09 2.13E+10
20 3.4384 3445 3.44E+06 3.15E+09 1.99E+10
+ + +
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. . . .
5 10 3.4980 3722 3.72E+06 3.33E+09 2.04E+10
20 3.4201 3445 3.44E+06 3.12E+09 1.91E+10
50 3.2714 3373 3.37E+06 3.06E+09 1.88E+10
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Customer Training Material Element Control
As stated earlier, the Solver Output reports the element technologybeing activated based on the element order chosen by user and thematerial association.
Elastic material or
metal plasticity withhigher order elements
2D Plane Stress/Strain
Metal Plasticity with
2D Plain Strain
Elastic material with
Fully incompressible
lower order elements
Simplified Enhanced Strain
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higher or lower order
elements B-Bar with Mixed u-P
ANSYS Mechanical Element Technology
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Customer Training Material Element Control
Users do have the option to turn Element Control off, thereby: Accepting the default technology
Receiving only suggestions in the Solution output with no changes.
The exception to this is Mixed u-P which must be turned on for fullyincompressible materials.
Refer also to ETCONTROL in Commands Manual
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Customer Training Material Element Control
With Element Control set to Manual, users can manually
toggle between Full and Reduced Integration Schemes
This switch only applies to higher order elements.
It is sometimes helpful to force full integration when only one
element exists across the thickness of a part. Doing this helps
prevent hour-glassing.
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Customer Training Material Element Control
Users can also override the default key option settings by executingthe following KEYOPT command within a command object under the
part branch. Recall:
KEYOPT, ITYPE, KNUM, VALUE
Where ITYPEis the Element type number
VALUEis the value of this KEYOPT
xamp e, e emen ype s , en ance s ra n can e
activated with the following command:
KEYOPT,1,1,2
Key Option Number (for element technology)
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Element Type Number
ANSYS Mechanical Element Technology
Summary
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Customer Training MaterialSummary
In summary, there are many different technologies forcontinuum elements to alleviate shearand volumetric locking
Unfortunatel , there is no silver bullet in circumventin mesh
locking, but Mechanical provides a wealth of element formulations,
so that users can balance accuracy, robustness, and efficiency insolving a wide range of nonlinear problems.
Lower-order elements can use B-Bar, URI, Enhanced Strain, or
Simplified Enhanced Strain. Moreover, Mixed u-P may be used in
conjunction with any of these formulations.
Higher-order elements usually use URI only (except for SOLID186,
which can also use full integration). Mixed u-P may be toggled on or
off, depending on the problem.
Mechanical will automatically set the best formulation option based
on the material properties and element order, although having an
understanding of the pros and cons of each formulation can be very
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.
The general recommendation is too accept these defaults
ANSYS Mechanical Element Technology
References for Further Reading
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Customer Training MaterialReferences for Further Reading
Some useful references on numerical theory:1. Non-Linear Finite Element Analysis of Solids and Structures Vol.1 and 2,
M.A. Crisfield, John Wiley & Sons, 1996 & 1997.
2. Nonlinear Continuum Mechanics for Finite Element Analysis, Bonet and
Wood, Cambridge University Press, 1997.3. Introduction to the Mechanics of a Continuous Medium, Malvern,
- , .
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