Dear Users,
I am modelling a special tower. There is a "beam" between the different floors which is actually made from steel plates. I have defined it as a user defined section. On the figure below you can see the section and how the columns attached with rigid links:
I set the Ux, Uy, Uz, and Rz blocked. However I am not sure in terms of moments and displacements that this is the correct approach to model the beam and the excentric columns' connection/ interaction. It looks like that in the model:
I have attached the example model as well. Please make a review and feedback how you would model such a beam column connection.
Thanks in advance!
Solved! Go to Solution.
Solved by Artur.Kosakowski. Go to Solution.
Solved by Rafacascudo. Go to Solution.
This might be stating the obvious but how about modelling the 'beam' as a plate element? or even multiple plate elements for a more realistic stiffness, or edit the plate properties for further realistic stiffness?
If you want to investigate local behavior, try modeling the connection as a solid.
That is OK , but I would make full rigid links and release the columns ends (if they need to) instead
Rafael Medeiros
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Thanks for the answer Rafacascudo !
Full rigid links mean that all the Ux, Uy, Uz and Rx, Ry, Rz are blocked, right? Maybe I misunderstood the rigid links, because I thought that with these blocked slave nodes the columns' ends wont be able to move or settle down, which wont be true. But it seems they can move, so what these blocked DoF means for the slave node?
If I release the columns end there are instabilities (Ux, Uz) during the calculation. What do you mean "if they need to" be released?
Thanks for your time and explanation in advance !
Rafael Medeiros
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Imagine a rigid link as a bar element which is e.g. 100 times more rigid than the ones it connects. The connection in its master node (let's name it origin) is fully fixed. The "releases" you define in its slave node (end) corresponds to a bar release (but this time you mark fixed these d.o.fs that you want to block) defined in the global coordinate system rather than in the local bar coordinate system.
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