The Beam Interface
The Beam interface (), found under the Structural Mechanics branch () when adding a physics interface, is used for modeling slender structural elements, having a significant bending stiffness. The formulation allows geometric nonlinearity, with large rotations and small strains, and beams can be modeled on 2D boundaries and 3D edges.
Two-noded straight elements with an Hermitian formulation are used. Two different assumptions about the physics can be used:
Among the computed results are displacements, rotations, stresses, strains, and section forces. In addition to giving the beam properties explicitly in terms of area, moment of inertia, and so on, several predefined common cross-section types are available. Cross section data to be used in Cross Section Data settings can be computed using Theory for the Beam Cross Section Interface.
The Linear Elastic Material node is the only available material model.
When this physics interface is added, these default nodes are also added to the Model Builder: Linear Elastic Material, Cross Section Data, Free (a condition where points are free, with no loads or constraints), and Initial Values. Then, from the Physics toolbar, add other nodes that implement, for example, loads and constraints. You can also right-click Beam to select physics features from the context menu.
Settings
The Label is the default physics interface name.
The Name is used primarily as a scope prefix for variables defined by the physics interface. Refer to such physics interface variables in expressions using the pattern <name>.<variable_name>. In order to distinguish between variables belonging to different physics interfaces, the name string must be unique. Only letters, numbers and underscores (_) are permitted in the Name field. The first character must be a letter.
The default Name (for the first physics interface in the model) is beam.
Beam Formulation
Select Euler-Bernoulli or Timoshenko to use the appropriate beam theory.
Backward Compatibility
This section only displays if a model was created in an earlier version. You also need to click the Show button () and select Advanced Physics Options to edit the section and change the Beam Formulation to Timoshenko (if required).
Click to clear the Use pre 4.4 formulation check box to convert a model into the new formulation. For most models, the only difference is that it will then be possible to select Timoshenko theory in the Beam Formulation section.
There are, however, some situations where you need to make additional changes to your model when migrating to the new formulation:
Reference Point for Moment Computation
Enter the default coordinates for the Reference point for moment computation xref. The resulting moments (applied or as reactions) are then computed relative to this reference point. During the results and analysis stage, the coordinates can be changed in the Parameters section in the result nodes.
Dependent Variables
The Beam interface has these dependent variables (fields):
The displacement field u, which has two components (u, v) in 2D and three components (u, v, and w) in 3D.
The rotation angle θ, which has one component in 2D (th) and three components in 3D (thx, thy, and thz).
The names can be changed but the names of fields and dependent variables must be unique within a model.
Discretization
The discretization cannot be changed. The element has different shape functions for the axial and transversal degrees of freedom. The axial displacement and twist are represented by linear shape functions, while the bending is represented by a cubic shape function (“Hermitian element”).
Channel Beam: Application Library path Structural_Mechanics_Module/Verification_Examples/channel_beam
Instability of a Space Arc Frame: Application Library path Structural_Mechanics_Module/Verification_Examples/
space_frame_instability