can be used to define interactions between bodies in mechanical, coupled
temperature-displacement, coupled thermal-electrical-structural, coupled pore
pressure-displacement, coupled thermal-electrical, and heat transfer simulations;
are part of the model definition;
can be formed using a pair of rigid or deformable surfaces or a single deformable
surface;
do not have to use surfaces with matching meshes;
cannot be formed with one two-dimensional surface and one three-dimensional surface; and
cannot be formed with cracked surfaces for enriched elements.
You can define contact in Abaqus/Standard in terms of two surfaces that may interact with each other as a “contact pair” or in terms
of a single surface that may interact with itself in “self-contact.” Abaqus/Standard enforces contact conditions by forming equations involving groups of nearby nodes from the
respective surfaces or, in the case of self-contact, from separate regions of the same
surface. This section describes various aspects of defining contact pairs and refers to other
sections for additional details.
To define a contact pair, you must indicate which pairs of surfaces may interact with one
another or which surfaces may interact with themselves. Contact surfaces should extend far
enough to include all regions that may come into contact during an analysis; however,
including additional surface nodes and faces that never experience contact may result in
significant extra computational cost (for example, extending a secondary surface such that
it includes many nodes that remain separated from the main surface throughout an analysis
can significantly increase memory usage unless penalty contact enforcement is used).
Every contact pair is assigned a contact formulation (either explicitly or by default) and
must refer to an interaction property. Discussion of the various available contact
formulations (based on whether the tracking approach assumes finite- or small-sliding—and
whether the contact discretization is based on a node-to-surface or surface-to-surface
approach) is provided in Contact Formulations in Abaqus/Standard. Interaction property
definitions are discussed in Assigning Contact Properties for Contact Pairs in Abaqus/Standard.
Defining Contact between Two Separate Surfaces
When a contact pair contains two surfaces, the two surfaces are not allowed to include
any of the same nodes and you must choose which surface will be the secondary and which
will be the main. The selection of main and secondary surfaces is discussed in detail in
Choosing the Main and Secondary Surface Roles in a Two-Surface Contact Pair. For
simple contact pairs consisting of two deformable surfaces, the following basic guidelines
can be used:
The larger of the two surfaces should act as the main surface.
If the surfaces are of comparable size, the surface on the stiffer body should act as
the main surface.
If the surfaces are of comparable size and stiffness, the surface with the coarser
mesh should act as the main surface.
The finite-sliding, node-to-surface formulation is used by default
(except in Abaqus/CAE, where the default is the finite-sliding, surface-to-surface formulation).
Defining Contact Pairs Using the Finite-Sliding, Node-to-Surface
Formulation
A finite-sliding, node-to-surface formulation is available.
Defining Contact Pairs Using the Finite-Sliding, Surface-to-Surface
Formulation
A node-based secondary surface precludes the use of surface-to-surface discretization.
Some contact capabilities are not available with the finite-sliding, surface-to-surface
formulation, including crack propagation (see Crack Propagation Analysis).
Defining Contact Pairs Using the Small-Sliding, Node-to-Surface Formulation
The small-sliding tracking approach uses node-to-surface discretization by default. For
an explanation of when the small-sliding tracking approach is appropriate in an
analysis, see Using the Small-Sliding Tracking Approach.
Defining Contact Pairs Using the Small-Sliding, Surface-to-Surface
Formulation
A node-based secondary surface precludes the use of surface-to-surface discretization.
Using Symmetric Main-Secondary Contact Pairs to Improve Contact Modeling
For node-to-surface contact it is possible for main surface nodes to penetrate the
secondary surface without resistance with the strict main-secondary algorithm used by Abaqus/Standard. This penetration tends to occur if the main surface is more refined than the secondary
surface or a large contact pressure develops between soft bodies. Refining the secondary
surface mesh often minimizes the penetration of the main surface nodes. If the refinement
technique does not work or is not practical, a symmetric main-secondary method can be used
if both surfaces are element-based surfaces with deformable or deformable-made-rigid
parent elements. To use this method, define two contact pairs using the same two surfaces,
but switch the roles of main and secondary surface for the two contact pairs. This method
causes Abaqus/Standard to treat each surface as a main surface and, thus, involves additional computational
expense because contact searches must be conducted twice for the same contact pair. The
increased accuracy provided by this method must be compared to the additional
computational cost.
All of the contact formulations are available for symmetric main-secondary contact pairs,
and can be applied using the same options discussed above.
Limitations of Symmetric Main-Secondary Contact Pairs
Using symmetric main-secondary contact pairs can lead to overconstraint problems when
very stiff or hard contact conditions are enforced. See Contact Constraint Enforcement Methods in Abaqus/Standard for a discussion of overconstraints and
alternate constraint enforcement methods.
For softened contact conditions, use of symmetric main-secondary contact pairs will
cause deviations from the specified pressure-versus-overclosure behavior, because both
contact pairs contribute to the overall interface stress without accounting for one
another. For example, symmetric main-secondary contact pairs effectively double the
overall contact stiffness if a linear pressure-overclosure relationship is specified.
Likewise, use of symmetric main-secondary contact pairs will cause deviations from the
friction model if an optional shear stress limit is specified (see Using the Optional Shear Stress Limit), because the contact stresses
observed by each contact pair will be approximately one-half of the total interface
stress.
Similarly, it can be difficult to interpret the results at the interface for symmetric
main-secondary contact pairs. In this case both surfaces at the interface act as
secondary surfaces, so each has contact constraint values associated with it. The
constraint values that represent contact pressures are not independent of each other.
Therefore, the constraint values reported in the data (.dat) and
results (.fil) files represent only a part of the total interface
pressure and have to be summed to obtain the total.
In the output database, mechanical contact variables are reported at the nodes on both
the main and secondary surfaces per contact pair and not just the secondary surface
where constraints are formed. Consequently, two result sets are available per surface of
a symmetric main-secondary contact pair; once when a surface acts as a secondary and
once as a main. For nodal contact pressures the Visualization
module of Abaqus/CAE only reports the maximum of the two pressure values associated with a node when the
surface containing the node acts either as a main or as a secondary surface. Even in
this case, the contact pressures do not represent the true interface pressure.
Apart from contact pressures, some contact output may be confusing with symmetric
main-secondary contact pairs. For example, Abaqus/Standard may report a positive opening distance on one side of a contact interface but zero
opening distance (i.e., touching) on the opposite side of the interface. Typically this
is caused by the shape or relative mesh refinement of the two surfaces.
Defining Self-Contact
Define contact between a single surface and itself by specifying only a single surface or
by specifying the same surface twice. The small-sliding tracking approach cannot be used
with self-contact.
Defining Self-Contact Using Node-to-Surface Discretization
Abaqus/Standard uses node-to-surface contact discretization by default for self-contact.
Defining Self-Contact Using Surface-to-Surface Discretization
Surface-to-surface discretization often leads to more accurate modeling of self-contact
simulations. However, because the self-contact surface is acting as both a main and a
secondary, surface-to-surface discretization can sometimes significantly increase the
solution cost.
Limitations of Self-Contact
Self-contact is valid only for mechanical surface interactions and is limited to finite
sliding with element-based surfaces.
A node of a self-contact surface can be both a secondary node and a member of the main
surface for two-dimensional self-contact using the surface-to-surface formulation and
for all three-dimensional self-contact. In these cases the contact behavior is similar
to symmetric main-secondary contact pairs, and the issues discussed in Using Symmetric Main-Secondary Contact Pairs to Improve Contact Modeling apply. Abaqus/Standard automatically applies some numerical softening to contact conditions
in these cases, as discussed in Contact Constraint Enforcement Methods in Abaqus/Standard.
Direct enforcement of hard contact conditions is the default constraint enforcement
method for two-dimensional self-contact using the node-to-surface formulation. In this
case, each node adjacent to a vertex where a two-dimensional surface folds onto itself
is automatically assigned a secondary or main role during the analysis. Since contact
constraints directly resist penetrations at nodes that act as secondary nodes, there is
some possibility of unresolved penetrations at nodes that only act as main nodes for
two-dimensional self-contact using the node-to-surface formulation.
Orientation Considerations for Shell-Like Surfaces
Abaqus/Standard requires main contact surfaces to be single-sided for node-to-surface contact and for
some surface-to-surface contact formulations (see Fundamental Choices Affecting the Contact Formulation for details).
This requires that you consider the proper orientation for main surfaces defined on
elements, such as shells and membranes, that have positive and negative directions. For
node-to-surface contact the orientation of secondary surface normals is irrelevant, but
for surface-to-surface contact the orientation of single-sided secondary surfaces is taken
into consideration.
Double-sided element-based surfaces are allowed for the default surface-to-surface
contact formulations, although they are not always appropriate for cases with deep initial
penetrations. If the main and secondary surfaces are both double-sided, the positive or
negative orientation of the contact normal direction will be chosen such as to minimize
(or avoid) penetrations for each contact constraint. If either or both of the surfaces are
single-sided, the positive or negative orientation of the contact normal direction will be
determined from the single-sided surface normals rather than the relative positions of the
surfaces.
When the orientation of a contact surface is relevant to the contact formulation, you
must consider the following aspects for surfaces on structural (beam and shell), membrane,
truss, or rigid elements:
Adjacent surface faces must have consistent normal directions. Abaqus/Standard will issue an error message if adjacent surface faces have inconsistent normals on
a single-sided surface whose orientation is relevant to the contact formulation.
Except for initial interference fit problems (see Modeling Contact Interference Fits in Abaqus/Standard), the secondary surface should be on the
same side of the main surface as the outward normal. If, in the initial configuration,
the secondary surface is on the opposite side of the main surface as the outward
normal, Abaqus/Standard will detect overclosure of the surfaces and may have difficulty finding an initial
solution if the overclosure is severe. An improper specification of the outward normal
will often cause an analysis to immediately fail to converge. Figure 1 illustrates the proper and improper specification of a main surface's outward
normal.
Contact will be ignored with surface-to-surface discretization if single-sided
secondary and main surfaces have normal directions that are in approximately the same
direction (for example, contact will not be enforced if the dot product of the
secondary and main surface normals is positive).
Initial clearances can be displayed in Abaqus/CAE with a contour plot of the variable
COPEN at increment 0 of the first
step; initial overclosures correspond to negative clearances.
Abaqus/Standard provides a detailed printout of the model's initial contact state.
Surface Connectivity Restrictions
Certain connectivity restrictions apply to contact surfaces depending on the type of
contact formulation. Surface connectivity restrictions for the various contact
formulations are summarized in Table 1. As indicated in this table, the connectivity restrictions are sometimes different for
main and secondary surfaces. Self-contact surfaces act as both main and secondary
surfaces; therefore, if a restriction applies to either a main or secondary surface, it
also applies to self-contact. The potential connectivity restrictions referred to in Table 1 are described below:
Table 1. Summary of which connectivity characteristics of element-based surfaces are allowed
for various contact formulations.
Contact formulation
Connectivity
characteristics
Discontinuous(or 3D faces joined at only one node)
T-intersection
Finite-sliding, node-to-surface
Main: Not allowedSecondary: Allowed
Main: Not allowedSecondary: Allowed
Small-sliding, node-to-surface
Main: AllowedSecondary: Allowed
Main: Not allowedSecondary: Allowed
Finite-sliding, surface-to-surface
Main: AllowedSecondary: Allowed
Main: AllowedSecondary: Allowed
Small-sliding, surface-to-surface
Main: AllowedSecondary: Allowed
Main: AllowedSecondary: Allowed
Discontinuous surfaces: Discontinuous contact surfaces are allowed in many cases, but
the main surface for finite-sliding, node-to-surface contact cannot be made up of two
or more disconnected regions (they must be continuous across element edges in
three-dimensional models or across nodes in two-dimensional models). Figure 2 shows examples of continuous surfaces, whereas Figure 3 and Figure 4 show examples of discontinuous surfaces. Figure 5 shows an automatically generated free surface resulting from the specification of
an element set consisting of two disjointed groups of elements. The resulting surface
is not continuous since it is composed of two disjoint open curves, so this surface
would be invalid as a main surface for finite-sliding, node-to-surface contact.
Portions of three-dimensional surfaces joined at only one node: The finite-sliding,
node-to-surface contact formulation also does not allow three-dimensional main surface
faces to be joined at a single node (they must be joined across a common element
edge). Figure 6 shows an example of a surface with two faces connected by a single node.
Surfaces with T-intersections: In some cases a contact surface cannot have more than
two surface faces sharing a common main node in two dimensions or a common main edge
in three dimensions. For example, Figure 7 shows examples of surfaces with T-intersections, in which three faces share a
common node in two dimensions or a common edge in three dimensions. While more than
two surface faces can share a common secondary node in two dimensions or a common edge
in three dimensions for node-to-surface formulations, the secondary faces must be
single-sided, which precludes the most common T-intersection cases for node-to-surface
formulations.
Analytical Rigid Surfaces
Analytical rigid surfaces are often effective for efficiently modeling curved, rigid
geometries, as discussed in Analytical Rigid Surface Definition. For rare cases
in which a very large number (thousands) of segments would be necessary to define an
analytical rigid surface, better performance can be achieved with an element-based rigid
surface (see Element-Based Surface Definition).
Three-Dimensional Beam and Truss Surfaces
Abaqus/Standard cannot use three-dimensional beams or trusses to form a main surface because the
elements do not have enough information to create unique surface normals. However, these
elements can be used to define a secondary surface. Two-dimensional beams and trusses can
be used to form both main and secondary surfaces.
Beam section offsets, specified either as part of the beam cross section definition or
through the BEAM SECTION OFFSET option, are
neglected for contact interactions in Abaqus/Standard.
Edge-Based Surfaces
Edge-based surfaces (Element-Based Surface Definition) on
three-dimensional shell elements cannot be used in a contact analysis in Abaqus/Standard.
Limitations of Node-Based Surfaces
Use node-based surfaces with caution when the contact property definition includes
user-defined softened contact properties or thermal or electrical interactions because the
contact constitutive behavior (which relies on accurate calculation of contact pressure,
heat flux, or electric current) will not be enforced correctly unless the precise surface
area is associated with each node. For details, see Contact Pressure-Overclosure Relationships, Thermal Contact Properties,
or Electrical Contact Properties.
Removing and Reactivating Contact Pairs
You can temporarily remove contact pairs from a simulation, which may result in significant
computational savings by eliminating unnecessary contact searches and updates of surface
orientations during the simulation. Removal and reactivation of contact pairs is commonly
used in complicated forming processes where multiple tools need to interact with the
workpiece at different stages in the analysis. Step-dependent activation and deactivation
are also supported for general contact when used as an alternative to contact pairs for
modeling contact (see Deactivating and Reactivating Contact Interactions across Steps).
Removal of contact pairs is a useful technique for uncoupling components of an assembly
until they should be brought together (such as tooling in manufacturing process
simulations). Significant computational expense might be saved by removing a contact pair
and introducing it at the proper time, thus eliminating the need to monitor the contact
conditions except when they are relevant.
Removal of Contact Forces Associated with Closed Contact Pairs
If the surfaces are in contact when a contact pair is removed, Abaqus/Standard stores the corresponding contact forces (or heat fluxes if thermal interactions are
present, or electrical currents if it is a coupled-thermal electrical analysis) for
every node on each surface. Abaqus/Standard automatically ramps these forces (or heat fluxes or electrical currents) linearly
down to zero magnitude during the removal step. Abaqus/Standard always removes the contact constraints for mechanical surface interactions
instantaneously.
Care must be taken in removing contact pairs in transient procedures. In transient heat
transfer, fully coupled temperature-displacement, or fully coupled
thermal-electrical-structural analysis if the fluxes are high and the step is long, this
ramping down may have the effect of cooling down or heating up the rest of the body. In
dynamic analysis if the forces are high and the step is long, kinetic energy can be
imparted to the remaining portion of the model. This problem can be avoided by removing
the contact pairs in a very short transient step prior to the rest of the analysis. This
step can be done in a single increment.
Using an Allowable Contact Interference to Deactivate Contact Pairs
A contact pair with mechanical contact interactions can be deactivated during an
analysis by assigning a very large allowable contact interference to the contact pairs
(see Modeling Contact Interference Fits in Abaqus/Standard). This method has the disadvantage
of not reducing the computational cost of the analysis because the contact algorithm
will still calculate the contact conditions for the contact pair in each increment.
Reactivating Contact Pairs
All contact pairs that will be used in a simulation must be created at the start of the
analysis; they cannot be created once the simulation has begun. However, contact pairs can
be created, removed at the start of the analysis in the first step, and then reactivated
at a later point during the simulation.
In Abaqus/CAE you can create contact pairs in any step. If a contact pair is created in a step other
than the initial step, Abaqus/CAE automatically deactivates the contact pair in the initial step and reactivates it in
the step in which you created it.
Reactivating Overclosed Contact Pairs
When a contact pair is reactivated, the contact constraint becomes active immediately.
In mechanical simulations it is possible for the surfaces of a contact pair to move such
that they become overclosed while the contact pair is inactive. If this overclosure is
too severe when the contact pair is reactivated, Abaqus/Standard may encounter convergence problems as it tries to enforce the suddenly activated
contact constraint. To avoid such problems, you can specify a permissible interference
value, v, for the contact pair that is larger than the overclosure
for the contact pair. Abaqus/Standard will ramp v down to zero during the step. For details on
specifying allowable interferences, see Modeling Contact Interference Fits in Abaqus/Standard.
Output
Output variables associated with the interaction of contact pairs fall into two categories:
nodal variables (sometimes called constraint variables) and whole surface variables. In
addition, Abaqus outputs an array of diagnostic information associated with contact interactions, as
discussed in Contact Diagnostics in an Abaqus/Standard Analysis.
For more detailed discussions of variables associated with
thermal, electrical, and pore fluid analyses, see the sections on the related contact
properties in Contact Property Models.
Nodal Contact Variables
Nodal contact variables can be contoured on contact surfaces in the
Visualization module of Abaqus/CAE. Nodal contact variables include contact pressure and force, frictional shear
stress and force, relative tangential motion (slip) of the surfaces during contact,
clearance between surfaces, heat or fluid flux per unit area, fluid pressure, and
electrical current per unit area. Many of the nodal contact variables written to the
output database (.odb) file are often available for all contact
nodes, regardless of whether they act as secondary or main nodes. Other nodal contact
variables are available only at nodes acting as secondary nodes. Most contact output to
the data (.dat) file, results (.fil) file, and
the utility subroutine GETVRMAVGATNODE is
associated with individual constraints. For contact output to the output database
(.odb) file, some filtering is applied to reduce contact output
noise.
The contact pressure distribution is of key interest in many Abaqus analyses. You can view the contact pressure on all contact surfaces except for
analytical rigid surfaces and discrete rigid surfaces based on rigid-type elements (the
latter restriction does not apply to general contact). You can view a contour plot of the
contact pressure error indicator next to a contour plot of the contact pressure to gain
perspective on local accuracy of the contact pressure solution in regions where the
contact pressure solution is of interest (see Selection of Error Indicators Influencing Adaptive Remeshing for further
discussion of error indicator output).
In some cases you may observe the contact pressure extending beyond the actual contact
zone due to the following factors:
The contour plots are constructed by interpolating nodal values, which can cause
nonzero values to appear within portions of facets outside of the contact region. For
example, this effect is often noticeable at corners, such as when two same-sized,
aligned blocks are in contact—if the contact surfaces wrap around the corners, the
contact pressure contours will extend slightly around the corners.
Abaqus/Standard outputs postprocessed contact stresses to the output database. During
postprocessing, nodal contact stresses are calculated as weighted averages of values
associated with active contact constraints in which the node participates. For
example, a main node can participate in multiple constraints whose connectivities
contain the node. Similarly, a secondary node can participate in multiple constraints,
as in the case of the finite sliding surface-to-surface formulation when more than one
constraint is created at secondary node locations that are corners and edge features.
The weighting depends on the contact constraint area and a scaling factor based on
the strength of the participation of the node in a constraint. The weighted averaging
is intended to reduce contact stress noise. Modifications are made for calculating
weightings, for example, at the corner nodes of quadratic faces (with zero consistent
nodal areas) and main nodes that are outside the active contact region but participate
in contact weakly through an active contact constraint. These modifications also have
a filtering effect in terms of reducing contact stress values reported for nodes on
the fringe of the active contact region. For such locations, contact nodal areas that
are simply cumulative scaled constraint areas across constraints in which a node
participates do not have much bearing on contact stress values.
In addition to averaging and filtering, contact stresses are also smoothed during the
postprocessing operations. However, this filtering and subsequent smoothing are not
"perfect" and can result in the contact zone size appearing somewhat exaggerated.
Similarly, contact status output is also affected at nodes that lie on the fringe of
the active contact region. In such cases, the contact status may be reported as closed
at nodes in the exaggerated region even though it is open.
Due to these factors, trying to infer the contact force distribution from the contact
stress distribution can be somewhat misleading. Instead, you can request nodal contact
force output, which accurately represents the contact force distribution present in the
analysis.
Whole Surface Variables
Whole surface variables are attributes of an entire secondary surface. Available as
history output, these variables record the total force and moment due to contact pressure
and frictional stress, the center of pressure and frictional stress (defined as the point
closest to the centroid of the surface that lies on the line of action of the resultant
force for which the resultant moment is minimal), and the total contact area (defined as
the sum of all the facets where there is contact force). The last letter of each variable
name (except the variable CAREA) denotes
which contact force distribution on the surface is used to calculate the resultant:
N
Normal contact forces are used to derive the resultant quantity.
S
Shear contact forces are used to derive the resultant quantity.
T
The sum of the normal and shear contact forces is used to derive the resultant
quantity.
For example, CFN is the total force due
to contact pressure, CFS is the total
force due to frictional stress, and CFT
is the total force due to both contact pressure and frictional stress.
Each total moment output variable will not necessarily equal the cross product of the
respective center of force vector and resultant force vector. Forces acting on two
different nodes of a surface may have components acting in opposite directions, such that
these nodal force components generate a net moment but not a net force; therefore, the
total moment may not arise entirely from the resultant force. The center of force output
variables tend to be most meaningful when the surface nodal forces act in approximately
the same direction.
Requesting Output
Certain contact variables must be requested as a group. For example, to output the
clearance between surfaces (COPEN), you
must request the variable CDISP (contact
displacements). CDISP outputs both
COPEN and
CSLIP (tangential motion of the surfaces
during contact). A complete listing of available contact pair variables and identifiers is
given in Abaqus/Standard Output Variable Identifiers.
Output requests can be limited to individual contact pairs or portions of a secondary
surface. You can:
request output associated with a given contact pair;
request output associated with a given secondary surface, including contributions
from all of the contact pairs to which the secondary surface belongs; and
limit the output by specifying a node set containing a subset of the nodes on the
secondary surface.
Instructions on forming these output requests are available in the following sections:
Differences for Small-Sliding and Finite-Sliding Contact
For small-sliding contact problems the contact area is calculated in the input file
preprocessor from the undeformed shape of the model; thus, it does not change throughout
the analysis, and contact pressures for small-sliding contact are calculated according to
this invariant contact area. This behavior is different from that in finite-sliding
contact problems, where the contact area and contact pressures are calculated according to
the deformed shape of the model.
Output of Tangential Results
Abaqus reports the values of tangential variables (frictional shear stress, viscous shear
stress, and relative tangential motion) with respect to the local tangent directions
defined on the surfaces. The local tangent directions
CTANDIR1 and
CTANDIR2 can be output by requesting the
generic output variable CTANDIR. The
definition of local tangent directions is explained in Local Tangent Directions on a Surface. These directions
do not always correspond to the global coordinate system, and they rotate with the contact
pair in a geometrically nonlinear analysis.
Abaqus/Standard calculates tangential results at each constraint point by taking the scalar product of
the variable's vector and a local tangent direction, or , associated with the constraint point. The number at the end of a
variable's name indicates whether the variable corresponds to the first or second local
tangent direction. For example, CSHEAR1
is the frictional shear stress component in the first local tangent direction, while
CSHEAR2 is the frictional shear stress
component in the second local tangent direction.
Definition of Accumulated Incremental Relative Motion (Slip)
Abaqus/Standard defines the incremental relative motion (also known as slip) as the scalar product of
the incremental relative nodal displacement vector and a local tangent direction. The
incremental relative nodal displacement vector measures the motion of a secondary node
relative to the motion of the main surface. The incremental slip is accumulated only
when the secondary node is contacting the main surface. The sums of all such incremental
slips during the analysis are reported as
CSLIP1 and
CSLIP2. Details about the calculation
of this quantity can be found in Small-sliding interaction between bodies, Finite-sliding interaction between deformable bodies, and Finite-sliding interaction between a deformable and a rigid body.
Extending the Range for Which Contact Opening Output Is Provided for Gaps
To reduce computational costs, detailed computations to monitor potential points of
interaction are avoided by default where surfaces are separated by a distance greater than
the minimum gap distance at which contact forces (or thermal fluxes, etc.) may be
transmitted. Therefore, contact opening
(COPEN) output is typically not provided
for finite-sliding contact where surfaces are opened by more than a small amount compared
to surface facet dimensions. You can extend the range in which Abaqus/Standard provides contact opening output;
COPEN will be provided up to gap
distances equal to a specified “tracking thickness.” Using this control may increase
computational cost due to extra contact tracking computations, especially if you specify a
large tracking thickness value.
Output for Axisymmetric Models
In an axisymmetric analysis the total forces and moments transmitted between the
contacting bodies as a result of contact pressure and frictional stress are computed in
the same manner as in a two-dimensional analysis. Therefore, the component of the total
forces along the r-axis is nonzero, and the components of the total
moments include contributions from the total forces along the r-axis.
Obtaining the “Maximum Torque” That Can Be Transmitted about the Z-Axis in an
Axisymmetric Analysis
When modeling surface-based contact with axisymmetric elements (element types
CAX and
CGAX), Abaqus/Standard can calculate the maximum torque (output variable
CTRQ) that can be transmitted about the
z-axis. This capability is often of interest when modeling threaded
connectors (see Axisymmetric analysis of a threaded connection). The maximum
torque, T, is defined as
where p is the pressure transmitted across the interface,
r is the radius to a point on the interface, and
s is the current distance along the interface in the
r–z plane. This definition of “torque”
effectively assumes a friction coefficient of unity.
Whole Model Contact-Related Energy Variables
For contact pairs, the same contact-related energy variables are available in Abaqus/Standard as for general contact, as described in Whole Model Contact-Related Energy Variables.