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Steel beam-column design to SANS 10162-1

A 203 × 203 × 46 H-section in S355, 4 m long, carrying 600 kN and 40 kNm: section class, column buckling, lateral-torsional buckling with Mcr, shear and the cl. 13.8 interaction. Every number below comes from the free STATIX steel member calculator and was checked by hand.

1. The problem

InputValue
Section203 × 203 × 46 H-section (universal column), hot-rolled
SteelS355: fy = 355 MPa, E = 200,000 MPa, G = 77,000 MPa
Length4.0 m, pinned both ends, K = 1.0 about both axes, braced frame
Design loads (ultimate, already factored)Cu = 600 kN, Mux = 40 kNm (major axis), Muy = 0, Vu = 120 kN
Lateral restraintnone between the ends: unbraced length for LTB = 4.0 m
Moment gradientω2 = 1.0 (uniform moment, the safe value); ω1 = 1.0

All resistance factors are φ = 0.9. Axes follow SANS 10162-1: x-x is the major axis, y-y the minor axis.

N-M interaction envelope for major-axis bending with the design point at 40 kNm and 600 kN, and the H-section shape, from the STATIX steel member calculator
The free steel member calculator with these inputs: the N–M envelope for major-axis bending, from Cr = 1,069 kN to Mr = 136 kNm, with the design point (40 kNm, 600 kN) at 89%.

2. Section properties

PropertyCalculator librarySAISC Red Book
A5,870 mm²5,880 mm²
h × b × tw × tf203.2 × 203.6 × 7.2 × 11.0 mm203.2 × 203.2 × 7.3 × 11.0 mm
Ix / Iy45.68 / 15.48 × 10⁶ mm⁴45.6 / 15.4 × 10⁶ mm⁴
Ze,x / Zpl,x450 / 497 × 10³ mm³449 / 497 × 10³ mm³
Ze,y / Zpl,y152 / 231 × 10³ mm³151 / 230 × 10³ mm³
rx / ry88.2 / 51.4 mm88.1 / 51.2 mm
J203 × 10³ mm⁴225 × 10³ mm⁴
CwIy(h − tf)²/4 = 143 × 10⁹ mm⁶142 × 10⁹ mm⁶

The two sets agree to within 1%, except the torsion constant J, which the library has about 10% below the Red Book. A lower J gives a lower Mcr, so the library value is on the safe side. With the Red Book values every result below changes by less than 1%.

3. Section class (SANS 10162-1 cl. 11, Table 4)

For the flange of an I-section the width b is half the full flange width (cl. 11.3.1c). The web width is the clear distance between the flanges (cl. 11.3.2c).

Flange: b/t = (203.6/2) / 11.0 = 9.25 Class 1 limit 145/√355 = 7.70, class 2 limit 170/√355 = 9.02, class 3 limit 200/√355 = 10.61 9.02 < 9.25 ≤ 10.61 → flange is class 3 Web: hw/tw = (203.2 − 2 × 11.0) / 7.2 = 25.2 Class 1 limit (1100/√355)(1 − 0.39 Cu/φCy) = 51.1 → web is class 1 Section: class 3 (the worst element governs)

Class 3 means the section reaches first yield but not the full plastic moment. Bending resistance is based on the elastic modulus Ze, not Zpl. Many H-sections in S355 are class 3 for this reason, while the same section in 300WA would be class 2.

4. Axial compression (cl. 13.3.1)

Cr = φ A fy (1 + λ2n)−1/n, n = 1.34 for hot-rolled sections λ = (KL/r) √(fy/(π²E)) Minor axis: KL/ry = 4,000 / 51.4 = 77.9 Fe = π² × 200,000 / 77.9² = 325.3 MPa, λy = √(355/325.3) = 1.045 Cry = 0.9 × 5,870 × 355 × (1 + 1.0452.68)−0.746 = 1,875.5 × 0.570 = 1,069 kN Major axis: KL/rx = 4,000 / 88.2 = 45.3, λx = 0.608 Crx = 1,875.5 × 0.840 = 1,575 kN Torsional buckling (cl. 13.3.2): fez = (π²ECw/L² + GJ) / (A r0²) = 544 MPa → Crz = 1,343 kN, does not govern Cr = 1,069 kN (minor axis) ≥ 600 kN OK (56%)

n = 2.24 applies only to welded three-plate members with flame-cut flange edges and to hot-formed or stress-relieved hollow sections. A rolled H-section always takes n = 1.34. The calculator uses 1.34 for every section, which is safe for the others.

5. Lateral-torsional buckling (cl. 13.6)

The compression flange is free over the full 4 m, so the moment resistance is limited by lateral-torsional buckling. For a class 3 section cl. 13.6(b) uses the yield moment My.

My = Ze,x fy = 450 × 10³ × 355 = 159.8 kNm, φMy = 143.8 kNm Mcr = (ω2 π / KL) √[ E Iy G J + (πE/KL)² Iy Cw ] E Iy G J = 200,000 × 15.48×10⁶ × 77,000 × 203×10³ = 4.84 × 10²² (πE/KL)² Iy Cw = (157.1)² × 15.48×10⁶ × 143×10⁹ = 5.46 × 10²² Mcr = 1.0 × π/4,000 × √(10.30 × 10²²) = 252.1 kNm Mcr = 252.1 > 0.67 My = 107.0 kNm, so Mrx = 1.15 φ My (1 − 0.28 My/Mcr) = 1.15 × 143.8 × (1 − 0.28 × 159.8/252.1) = 165.3 × 0.823 = 136.0 kNm (not more than φMy = 143.8) Mux = 40 kNm ≤ 136.0 kNm OK (29%)

ω2 = 1.0 is the value for uniform moment, the worst case. If the moment varies linearly between the ends, cl. 13.6(a) gives ω2 = 1.75 + 1.05κ + 0.3κ² ≤ 2.5. Here κ is the ratio of the smaller to the larger end moment, positive for double curvature and negative for single curvature. Uniform moment is κ = −1 and gives ω2 = 1.0. A beam with one end moment zero is κ = 0 and gives 1.75. Getting the sign wrong turns 1.0 into 2.5.

6. Minor-axis bending (cl. 13.5)

There is no minor-axis moment in this example, but the resistance is still reported. For a class 3 section cl. 13.5(b) uses the elastic modulus about both axes.

Mry = φ Ze,y fy = 0.9 × 152 × 10³ × 355 = 48.6 kNm

7. Shear (cl. 13.4.1.1)

Av = h tw = 203.2 × 7.2 = 1,463 mm² (rolled section) hw/tw = 25.2 ≤ 440 √(kv/fy) = 440 √(5.34/355) = 54.0 → no shear buckling fs = 0.66 fy = 234.3 MPa Vr = φ Av fs = 0.9 × 1,463 × 234.3 = 308.5 kN ≥ 120 kN OK (39%)

kv = 5.34 is the value for a web without transverse stiffeners.

8. Axial load and bending (cl. 13.8.3)

The section is class 3, so cl. 13.8.3 applies (all sections except class 1 and class 2 I-shapes). Its coefficients are 1.0 on both moment terms. Class 1 and 2 I-shapes use cl. 13.8.2 with 0.85 and β.

Cu/Cr + U1x Mux/Mrx + U1y Muy/Mry ≤ 1.0 Amplification (cl. 13.8.4): Cex = π²E Ix/L² = π² × 200,000 × 45.68×10⁶ / 4,000² = 5,636 kN U1x = ω1 / (1 − Cu/Cex) = 1.0 / (1 − 600/5,636) = 1.119 (a) Cross-section: Cr at λ = 0 = φAfy = 1,875.5 kN, Mrx = φMy = 143.8 kNm, U1x ≥ 1.0 600/1,875.5 + 1.119 × 40/143.8 = 0.320 + 0.311 = 0.63 (b) Overall member: Cr = Cry = 1,069 kN, Mrx = 143.8 kNm 600/1,069 + 1.119 × 40/143.8 = 0.561 + 0.311 = 0.87 (c) Lateral-torsional buckling: Cr = Cry = 1,069 kN (weak axis), Mrx = 136.0 kNm (cl. 13.6), U1x ≥ 1.0 600/1,069 + 1.119 × 40/136.0 = 0.561 + 0.329 = 0.89 ← governs 0.89 ≤ 1.0 OK

Case (c) governs, as it usually does for an unrestrained column in bending: the weak-axis buckling load and the LTB moment are both the lowest values of their kind. U1x = 1.119 means the 40 kNm grows by about 12% from the member's own deflection under 600 kN.

In case (b) the calculator uses the weak-axis Cr. For bending about the strong axis only, cl. 13.8.2(b) lets you use Cr = Crx = 1,575 kN, which gives 0.381 + 0.311 = 0.69. The calculator's 0.87 is on the safe side, and case (c) governs either way.

9. Result

CheckResult
Section classClass 3 (flange b/t = 9.25 > 9.02)
Axial compression600 ≤ 1,069 kN (56%)
Major-axis bending with LTB40 ≤ 136.0 kNm (29%), Mcr = 252 kNm
Minor-axis bending resistance48.6 kNm (no demand)
Shear120 ≤ 308.5 kN (39%)
Interaction, cl. 13.8.3(c)0.89 ≤ 1.0
Mass46.1 kg/m × 4.0 m = 184 kg

The member works at 89%. The two cheap ways to more capacity are a lateral restraint at mid-height (halves the LTB and weak-axis lengths) and a real ω2 if the moment is not uniform.

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