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Lateral Torsional Buckling of Hollow Steel Sections 1

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EV11

Structural
Mar 30, 2021
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CA
Hi everyone,

Question from a young engineer in training from Canada – can a symmetrical hollow section (square in my case) undergo lateral torsional buckling? Do the out-of-plane stability design checks for beam-columns apply to symmetrical hollow sections?

I am working on the design of an exterior corner column (hollow square section, 14-feet high) in a structural steel building that is subject to bi-axial bending. When verifying out-of-plane stability (lateral torsional buckling) I am obtaining strange results. One issue is the warping constant. I have not found much information on the warping constant for hollow sections. Logically, it would make sense for it to be negligible or zero, I just want to make sure that I am not overlooking anything.

Any information or explanations would be appreciated.

Thank you.
 
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Warping constant is zero for closed hollow sections.

I don't have my code in front of me, but if I remember correctly they don't explicitly require LTB checks for closed hollow squares. I believe in 13.6 (laterally unsupported) it says for closed square and circular sections you just check it as per 13.5 (laterally supported)
 
For a square HSS beam? I don't think LTB is possible. You'd have to have something like a really tall rectangular HSS with a short width to cause any LTB in an HSS. Even then, I'm not sure.

The key is that you need the weak axis buckling and torsional stiffness of the beam to be significantly lower compared to strong axis in order to have LTB. It just doesn't happen with HSS.
 
Hi,

In my view you check regular bending/deflection/shear. A hollow section won’t buckle LTB style - unless you’re into some totally obscure slender plate girder that’s massively disproportionate of course which I assume you’re not.
 
We had some fun investigating the likelihood of LTB in tubes here: Link. The sketch below is some of my hyperbolic handiwork from that one exploring the possibility of LTB in a section bending about its weak axis. In summary:

1) Theoretically, you can LTB anything.

2) Practically, it's very difficult to LTB an HSS until the [Ix:Iy] ratio starts to get high.

OP said:
I have not found much information on the warping constant for hollow sections. Logically, it would make sense for it to be negligible or zero

This raises another interesting point of pedantry. While the the warping constant for closed sections is often taken as zero:

1) It is, in fact, not zero.

2) It's actually more than a comparable wide flange.

3) I believe that it is truly zero only for circular cross sections.

3) We take it as zero simply because, for a closed section with a modest [Ix:Iy] ratio, the St.Venant torsional stiffness skyrockets and dominates the expression for torsional stiffness. It's just a convenient way to zero out the term that accounts for warping torsional stiffness.


C01_t1zlsc.jpg
 
An SHS can’t avoid work by buckling, thus it won’t buckle.

It’s an interesting question as to what the slenderness cut off is for hollow sections. How narrow do they have to get for it to be easier for them to buckle than to keep on bending...
 
The latest AISC spec has LTB buckling capacity formulations for both SHS and RHS. So one need no longer resort to H:W rules of thumb which I've encountered in the rang of 2.0 to 4.0.
 
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