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Typical applications for coupled DOFs include: 1) maintaining symmetry on partial models, 2) forming pin, hinge, universal, and slider joints between two coincident nodes, and 3) forcing portions of your model to behave as rigid bodies (see this chapter's discussion of constraint equations for more general rigid region capability).
Command(s):
Main Menu>Preprocessor>Coupling / Ceqn>Couple DOFs
After creating a coupled set of nodes, you can include more nodes in that set by simply performing an additional coupling operation (be sure to use the same set reference number). You can also use selecting logic to couple "ALL" of the selected nodes. Nodes can be deleted from a coupled set by inputting them as negative node numbers on the CP command. To modify a coupled DOF set (that is, add or delete nodes, or change the DOF label), use the CPNGEN command. (You cannot access the CPNGEN command directly in the GUI.)
Command(s):
Main Menu>Preprocessor>Coupling / Ceqn>Coincident Nodes
Instead of coupling coincident nodes, you can use one of these alternative methods to force the nodes to behave in the same way:
Main Menu>Preprocessor>Coupling / Ceqn>Gen w/Same Nodes
Main Menu>Preprocessor>Coupling / Ceqn>Gen w/Same DOF
Utility Menu>List>Other>Coupled Sets>All CP nodes selected
Utility Menu>List>Other>Coupled Sets>Any CP node selected
Main Menu>Preprocessor>Coupling / Ceqn>Del Coupled Sets
Degrees of freedom are coupled within a set but are not coupled between sets. You must not allow a degree of freedom to appear in more than one coupled set.
"Grounded" degrees of freedom (that is, DOFs with values specified by D or other constraint commands) must not be included in the coupled set.
In a reduced analysis, if master degrees of freedom are to be chosen from coupled DOF sets, only prime DOFs may be designated as master degrees of freedom. (You must not designate any eliminated DOF in a coupled set as a master degree of freedom.)
In a structural analysis, coupling DOFs to create a rigid region can sometimes cause apparent violations of equilibrium. A set of coupled nodes which are not coincident or are not in line with the coupled displacement direction may produce an applied moment that will not appear in the reaction forces.
where U(I) is the degree of freedom of term (I), and N is the number of terms in the equation.
Command(s):
Main Menu>Preprocessor>Coupling / Ceqn>Constraint Eqn
The following example illustrates a typical application of a constraint equation, in which moment transfer capability is created for a connection between a BEAM3 element and PLANE42 elements (PLANE42 elements have no in-plane rotational degree of freedom):
Figure 12-1 Establishing relationships between rotational and translational degrees of freedom
In this example, node 2 acts as a hinge if no constraint equations are used. To transfer moment between the beam and the plane-stress elements, you can use the following equation:
ROTZ2 = (UY3 - UY1)/10
This equation would be rewritten in the required format and entered into the program as:
0 = UY3 - UY1 - 10*ROTZ2
CE,1,0,3,UY,1,1,UY,-1,2,ROTZ,-10The first unique degree of freedom in the equation is eliminated in terms of all other degrees of freedom in the equation. A unique degree of freedom is one which is not specified in any other constraint equation, coupled node set, specified displacement set, or master degree of freedom set. You should make the first term of the equation be the degree of freedom to be eliminated. Although you may, in theory, specify the same degree of freedom in more than one equation, you must be careful to avoid over-specification. You must also take care to ensure that each node and degree of freedom exists in the model. (Remember that for a degree of freedom to be present at a node, that node must be connected to an element which supplies the necessary degree of freedom.)
A periodic condition is a boundary for which neither the flux-parallel nor flux-normal conditions hold, but rather the potential at one point is of equal magnitude but of opposite sign to that of a point in another location. This condition arises in the analysis of symmetry sectors of motors, for example, where the potentials one pole pitch apart are equal but opposite in sign. In Figure 12-2, suppose node 129 in the outlined symmetry sector is to be constrained as described above with node 363 on the opposite pole pitch.
Figure 12-2 Example of specifying a periodic condition
The constraint equation would read:
The CE command used to input this constraint equation would appear as follows:
CE,1,0,129,MAG,1,363,MAG,1To automatically apply groups of periodic boundary conditions (CP and CE commands) for 2-D magnetic analyses, use the PERBC2D command macro (refer to Chapter 11 of the ANSYS Electromagnetic Field Analysis Guide for a discussion of this modeling aide):
Command(s):
Main Menu>Preprocessor>Loads>Apply>Periodic BCs
Main Menu>Solution>Apply>Periodic BCs
Note-Periodic boundary conditions can also be represented in a structural analysis (for example, in a turbine blade model) using CP commands on nodes rotated into the cylindrical coordinate system.
Command(s):
Main Menu>Preprocessor>Coupling / Ceqn>Modify ConstrEqn
Main Menu>Preprocessor>Loads>Other>Modify ConstrEqn
Main Menu>Solution>Other>Modify ConstrEqn
If you need to change any of the other terms of a constraint equation, you must use the CE command (or the corresponding GUI path) in PREP7, before you start your solution.
Three other operations, described below, automatically generate multiple constraint equations for you.
Command(s):
Main Menu>Preprocessor>Coupling / Ceqn>Rigid Region
By setting Ldof to ALL on the CERIG command (default), this operation will generate three equations for each pair of constrained nodes in 2-D space. These equations define the three rigid body motions in global Cartesian space (UX, UY, ROTZ). In order to create a rigid region on a 2-D model, you must make sure that the X-Y plane is the rigid plane and that UX, UY, and ROTZ degrees of freedom are available at each constrained node. This operation will similarly generate six equations for each pair of constrained nodes in 3-D space. All six degrees of freedom (UX, UY, UZ, ROTX, ROTY, and ROTZ) must be available at each constrained node.
Entering other labels in the Ldof field will create different effects. If this field is set to UXYZ, the program will write two constraint equations in 2-D (X,Y) space and three constraint equations in 3-D (X,Y,Z) space. These equations will be written in terms of the slave nodes' translational degrees of freedom, and in terms of the master node's translational and rotational degrees of freedom. Similarly, the RXYZ label allows you to generate a partial set of equations that omit the slave nodes' translational degrees of freedom. The other available Ldof labels will generate other types of constraint equations.
In general, your slave nodes need have only the degrees of freedom called for by Ldof, but your master node must have all applicable translational and rotational degrees of freedom (that is, UX, UY, ROTZ for 2-D; UX, UY, UZ, ROTX, ROTY, ROTZ for 3-D). For models that are made up of elements having no rotational degree of freedom, you might consider adding a dummy beam element to provide rotational degrees of freedom at the master node.
Certain limitations affect the CEINTF command: stress or thermal flux might not be continuous across the interface. Nodes in the interface region must not have specified displacements. You can interface 6-DOF solids only with other elements having six degrees of freedom per node.
Command(s):
Main Menu>Preprocessor>Coupling / Ceqn >Gen w/same DOF
Utility Menu>List>Other>Constraint Eqns>All CE nodes selected
Utility Menu>List>Other>Constraint Eqns>Any CE node selected
Main Menu>Preprocessor>Coupling / Ceqn>Del Constr Eqn
The presence of constraint equations can produce unexpected reaction and nodal force results. Please see the related discussion in Chapter 5 of the ANSYS Basic Analysis Procedures Guide.