Summary
In this lecture, we will cover the following:
- We will define a drilling degree of freedom as rotation about the element normal,
- We will see why co-planar connected elements can leave drilling rotations unrestrained,
- We will start linking drilling degrees of freedom with stiffness matrix singularity.
We start by returning to the local element reference frame, where each shell node has five degrees of freedom: membrane displacements, transverse displacement, and two rotations. When the element is placed into the global structure, rotations are expressed relative to the global axes, and this leads to a sixth rotational degree of freedom at every node.
We then identify this extra rotation as the drilling degree of freedom: a rotation about the element normal. Because the local shell formulation does not include stiffness associated with this rotation, the element provides no resistance to it. When co-planar elements share nodes, these drilling rotations can remain unrestrained, creating the conditions for a singular stiffness matrix.
Next up
In the next lecture, we will make this connection more precise by looking directly at what stiffness matrix singularity means.
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Finite Element Analysis of Plate and Shell Structures: Part 2 - Shells
Expanding from plate to shell elements - build a workflow that unlocks the behaviour of 3D shell structures
After completing this course...
- You will understand how we make the leap from Reissner-Mindlin plate elements to shell elements and what extra modelling fidelity that provides.
- You will be comfortable using a combination of GMSH and the open-source 3D modelling software, Blender, to generate custom finite element meshes.
- You will be able to use OpenSeesPy to model shell structures, as an alternative to your own custom finite element solver.
- You will have a much greater understanding of what commercial finite element packages are doing, behind the UI, allowing you to authoritatively interrogate their results.
