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Unstiffened RHS mitre joint 1

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bugbus

Structural
Aug 14, 2018
533
I am trying to model the plastic collapse load for an unstiffened RHS mitre joint using Strand7 (unstiffened in the sense that there is no diagonal end plate welded between the two RHS sections - the two RHSs are simply mitre cut and butt welded together and the joint is hollow all the way through).

I just want to check that my general approach is OK.

The section is a 150x100x5.0 RHS, fy = 450 MPa, fu = 500 MPa. For reference, the plastic section capacity is 52 kNm.

The model consists of 8-node curved plate elements (mostly), although the auto-mesh feature occasionally includes some 6-node triangles here and there. Meshing is more refined around the inside corners where the stress tends to concentrate. The straight portion away from the joint is about 150 mm long, equal to the height of the section. I've used a multi-node link at each end, one with fixed boundary conditions, and the other set to rotate 0.05 degrees about the major axis so that the joint is opening.
1_ufe0zw.png

2_s5jxas.png


The stress-strain curve is shown below:
3_cvmnfz.png


The model runs fine up until the 8th time step (i.e. for an imposed rotation of 8 x 0.05 = 0.40 degrees), at which point it struggles to converge on a solution. My main reference for this type of joint says that the capacity should reach approximately 50% of the section capacity, i.e. 50% x 52 kNm ~ 26 kNm.

However, you can see on the graph below (bending moment [kNm] vs rotation [degrees]) that it doesn't seem to approach any sort of collapse mechanism, there is only a hint of non-linear behaviour as the rotation approaches 0.4 degrees.
6_sgfc8x.png


Below is showing the yielded areas at rotations of 0.30, 0.35 and 0.40 (not converged) degrees.
44_fxshp9.png

4_kqobch.png

5_rqgppz.png


This seems to confirm that the collapse mechanism is not even close to being reached. The yielding is only occurring locally around the corners of the joint.

There are no odd stress concentrations or deformations occurring around the multi-node links, so I'm confident this isn't the issue.

Is it simply a case of the 'load' step being too large? Should I just set this to be smaller and leave it to run for longer? Any other suggestions?
 
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this is two pieces welded together, yes ? How are you modelling the weld ?

have you tests to compare to ?

"Hoffen wir mal, dass alles gut geht !"
General Paulus, Nov 1942, outside Stalingrad after the launch of Operation Uranus.
 
you have modelled a sharp corner which induces a singularity; in reality the welded joint is not a sharp corner.
 
Are there any good articles on this type of design problem, not using FEM?

-----*****-----
So strange to see the singularity approaching while the entire planet is rapidly turning into a hellscape. -John Coates

-Dik
 
rb1957 - simply by connecting the plates where they intersect. There is no special weld element modelled. I don't have tests to compare it to, but I know that the ballpark figure should be about 1/2 of the section capacity of a straight member based on one of the Australian Steel Institute design guides.

SWComposites - you're correct, it is a sharp point, particularly at that concave portion at the inside of the joint, which is where I am getting the large stress concentration. I hadn't really considered that as a problem before, but this is something I might look into. Do you know whether the nonlinear material in my model would help to 'relieve' that stress concentration in the model and avoid this as an issue?

dik - the reference I'm considering is one of the Australian Steel Institute design guides (which I don't have in front of me unfortunately). I think they go into pretty good detail about how this joint collapses, which is where they derive the ~50% number from. For reference, with a stiffener plate welded between, I recall that the capacity is close to 100% (if not 100%).
 
Also, @rb1957 and @SWComposites, the model was generated from a dxf file that I created in Autocad - see below. You can see the sharp corner along the edge where the two sections intersect. In reality, yes, there would be some rounding along this edge where it would be welded.

1_piemeb.png
 
maybe you should model a radius at the corner that is representative of the weld geometry.

further, how are you accounting for the different properties of the weld material?
 
Thanks, I'll try that out. Not sure about the second part of your comment, the weld strength used (fu = 490 MPa) would be very similar to the strength of the tube (fu = 500 MPa). I would be tempted to use the same material all the way through unless you can think of a reason not to?
 
i'm not a weld expert, but the weld material stress-strain response and HAZ material stress-strain response might be different than the base material stress-strain response, which could be important if you are running a nonlinear FEM.
 
Great, thanks again, will report back if I have any luck
 
well SWC reiterated my points, and at least you replied more sensibly to him. Modelling the section with plates is fine, but you're not capturing critical features of the analysis.

To learn how to model welds I think you need a set of test data to info how to build the model. "fussing" over the profile of the weld will only beguile you into believing the results of the FEM. I would expect that you can get a long way modelling with plates, but I would expect that the weld could be modelled by a CBUSH (well, that's the NASTRAN element for some sort of spring ... STRAND7 has never impressed me, from what I've read about it here). And to get anywhere near right, you'll need to run material (and maybe geometry) non-linear.

"Hoffen wir mal, dass alles gut geht !"
General Paulus, Nov 1942, outside Stalingrad after the launch of Operation Uranus.
 
I've figured out how to round the edges, which gives me the below mesh (there are a few oddly shaped elements, but I'm just testing if there's any improvement). So far, it seems to be working, just very slow to converge on a solution. I will run it overnight and see what it gives me.

I am running material and geometry nonlinearity.

1_d6kcmw.png
 
Thanks so much...

-----*****-----
So strange to see the singularity approaching while the entire planet is rapidly turning into a hellscape. -John Coates

-Dik
 
gusmurr - have you performed a simple hand analysis to compare to the STI equation? shouldn't be too hard to calc the stress at the inner corner and make an estimate of strength using plasticity analysis.
 
What is the plate element? Kirchoff or Reissner-Mindlin? If Reissner-Mindlin, are the elements locking-free? You want a Kirchoff element or a locking-free RM element for your plates.

How is geometric non-linearity modelled: is it a von Karman type non-linearity (quadratic order strains for the kinematics, moderate rotations), or a finite strain and finite displacement formulation that solves the system based on deformed geometry? Is the geometrical non-linearity non-locking, i.e., is the formulation such that no membrane locking or shear locking can occur?

What is the solver? Is it a Newton-Raphson or modified Newton-Raphson solver with force control (those do not converge for non-monotonic stress-strain or load-displacement behavior), or an arc-length method with displacement control (should converge for almost any type of problem with small enough displacement increments and enough iterations per displacement increment), or something else?

How is the material modelling performed? The stress-strain curve you show is not very realistic and seems to be based on some rough zero-hardening idealization found in a code.

Non-linear finite element analysis is really quite complicated, and many softwares with NL FEA do not offer a robust and reliable procedure for it. Quite a lot can go wrong, and rarely will customer support admit to the software being unreliable. I am not familiar with Strand7, but I am quite certain that at least ABAQUS and ANSYS can solve this problem and both have user manuals and customer support which will not actively try to hide the details (elements, locking behaviour, kinematics, material modelling, solvers etc.) of their product.
 
The anaysis is a little tricky because of the 'crushing' wall strength of the HSS at the reentrant corner.

-----*****-----
So strange to see the singularity approaching while the entire planet is rapidly turning into a hellscape. -John Coates

-Dik
 
SWComposites - yes I have, I get roughly the same capacity as that equation.

@centondolar - I can't answer all your questions, but I'll try. I believe the plates are Kirchoff; I have since removed the geometric nonlinearity as it was slowing down the solver and I don't think it's necessarily relevant in this case; arc-length method; you're correct about the stress-strain curve, this isn't necessarily realistic.


I have since simplified things a bit. I split the model into 1/4 of the previous and included symmetry conditions, removed the geometric nonlinearity, and made the mesh a bit coarser. This seems to get the solver to work in a more reasonable time.
2_uyapfp.png


Doing some more reading on the topic (e.g. tests by Wilkinson and Hancock ca. 1998, there's plenty of papers out there), joints of this type tend to fail by tearing of the tube or failure of the weld in the highly stressed corner shown above.
4_wwwwoy.png


This occurs well before a complete collapse mechanism is able to form. My results tend to show this as well - below you can see that when the strain in the tube starts to exceed about 5%, this is where the theoretical capacity occurs.
3_nnuf1b.png


Anyway, I think I'm done with this little exercise for now. Thanks for the comments everyone.
 
OK, last comment and I promise I'll be done.

Interesting excerpts from one of the papers I read - 'Tests of knee joints in cold-formed rectangular hollow sections' by Wilkinson and Hancock 1998.

(My highlights added for emphasis)
5_ppy6ag.png


Fracture at the corner of the RHS occurs at around 5% strain.
6_lknd5f.png
 
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