Defining a Local Coordinate System
Normally displacement and rotation components are associated with the global, rectangular Cartesian axis system. When a transformed coordinate system is associated with a node, all input data for concentrated forces and moments and for displacement and rotation boundary conditions at the node are given in the local system. The following transformations are available:
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Rectangular Cartesian
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Cylindrical
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Spherical
The coordinate transformation defined at a node must be consistent with the degrees of freedom that exist at the node. For example, a transformed coordinate system should not be defined at a node that is connected only to a SPRING1 or SPRING2 element, since these elements have only one active degree of freedom per node.
Defining a Local Coordinate System in a Model That Contains an Assembly of Part Instances
In a model defined in terms of an assembly of part instances, you can define a nodal transformation at the part, part instance, or assembly level. A nodal transformation defined at the part or part instance level will be rotated according to the positioning data given for each instance of that part (or for the part instance). See Assembly Definition. Multiple transformation definitions are not allowed at a node, even if one of them is at the part level and another is at the assembly level.
Large-Displacement Analysis
The transformed coordinate system is always a set of fixed Cartesian axes at a node (even for cylindrical or spherical transforms). These transformed directions are fixed in space; the directions do not rotate as the node moves. Therefore, even in large-displacement analysis, the displacement components must always be given with respect to these fixed directions in space.
Defining a Rectangular Cartesian Coordinate Transformation
In a rectangular Cartesian transformation the transformed directions are parallel at all nodes of the set. The coordinates of two points must be given, as shown in Figure 1.
The first point, a, must be on a line through the global origin; this point defines the transformed -direction. The second point, b, must be in the plane containing the global origin and the transformed - and -directions. This second point should be on or near the positive -axis.
Defining a Cylindrical Coordinate Transformation
The radial, tangential, and axial directions must be defined based on the original coordinates of each node in the node set for which the transformation is invoked. The global () coordinates of the two points defining the axis of the cylindrical system (points a and b as shown in Figure 2) must be given.
The origin of the local coordinate system is at the node of interest. The local -axis is defined by a line through the node, perpendicular to the line through points a and b. The local -axis is defined by a line that is parallel to the line through points a and b. The local -axis forms a right-handed coordinate system with and .
A cylindrical coordinate system cannot be defined for a node that lies along the line joining points a and b.
Defining a Spherical Coordinate Transformation
The radial, circumferential, and meridional directions must be defined based on the original coordinates of each node in the node set for which the transformation is invoked. The global () coordinates of the center of the spherical system, a, and of a point on the polar axis, b, must be given as shown in Figure 3.
The origin of the local coordinate system is at the node of interest. The local -axis is defined by a line through the node and point a. The local -axis lies in a plane containing the polar axis (the line between points a and b) and is perpendicular to the local -axis. The local -axis forms a right-handed coordinate system with and .
A spherical coordinate system cannot be defined for a node that lies along the line joining points a and b.