Hollow Section Design Theory - CHS, SHS, RHS (Eurocode 3)

Hollow sections - circular (CHS), square (SHS) and rectangular (RHS) - are closed profiles whose behaviour differs fundamentally from open sections.

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Closed sections and torsion

A closed (hollow) section is enormously stiffer in torsion than an open one of the same size - by orders of magnitude. This makes hollow sections the natural choice wherever torsion or biaxial loading matters, and means lateral-torsional buckling is rarely critical for them.

Compression performance

Square and circular hollow sections have equal (or near-equal) radii of gyration about both axes, so there is no weak axis - buckling resistance is the same in every direction. Combined with their high torsional stiffness, this makes SHS/CHS very efficient columns, and they are widely used architecturally for their clean appearance.

Hot-finished vs cold-formed

Hot-finished hollow sections (EN 10210) have uniform properties and sharper corner geometry; cold-formed (EN 10219) are formed at ambient temperature, with work-hardened, more rounded corners and slightly different design parameters. The tool lists both - check which standard a project specifies.

Combined axial + bending (interaction)

Hollow-section beam-columns are verified by the cross-section interaction (§6.2.9), where axial load n=NEd/Npl,Rdn=N_{Ed}/N_{pl,Rd} reduces the moment resistance to MN,RdM_{N,Rd}, and the member stability check (§6.3.3). Both Expressions (6.61) and (6.62) must be satisfied:

NEdNb,y,Rd+kyyMy,EdMb,Rd+kyzMz,EdMc,z,Rd1.0(6.61)\frac{N_{Ed}}{N_{b,y,Rd}} + k_{yy}\frac{M_{y,Ed}}{M_{b,Rd}} + k_{yz}\frac{M_{z,Ed}}{M_{c,z,Rd}} \le 1.0\quad(6.61)
NEdNb,z,Rd+kzyMy,EdMb,Rd+kzzMz,EdMc,z,Rd1.0(6.62)\frac{N_{Ed}}{N_{b,z,Rd}} + k_{zy}\frac{M_{y,Ed}}{M_{b,Rd}} + k_{zz}\frac{M_{z,Ed}}{M_{c,z,Rd}} \le 1.0\quad(6.62)

Because closed sections are not susceptible to torsional deformation, the Annex B factors take their simpler Table B.1 form (kzy=0.6kyyk_{zy}=0.6\,k_{yy}), and the kzzk_{zz} form for RHS uses Cmz[1+(λˉz0.2)nz]C_{mz}\,[1+(\bar\lambda_z-0.2)\,n_z] rather than the I-section expression. For SHS and CHS there is no lateral-torsional buckling, so Mb,Rd=Mc,RdM_{b,Rd}=M_{c,Rd} in the equations above. The worked example evaluates the factors and both expressions for a representative section.

Section tables
CHSSHSRHSEHSCHS-CFSHS-CFRHS-CF

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