Area, second moment of area, elastic section modulus and radius of gyration for nine common cross-sections, with the axis each value refers to stated.
Data verified 2026-09-29 · based on AISC 15th edition (2017), Shapes Database v15.0
| Cross-section[2] | Axis the values refer to[2] | Area, A[1] | Second moment of area, I[1] | Elastic section modulus, S[1] | Radius of gyration, r[1] |
|---|---|---|---|---|---|
| Rectangle, b × h # | Bending about the centroidal axis parallel to b | A = b·h | b·h³ ÷ 12 | b·h² ÷ 6 | h ÷ √12 = 0.2887h |
| Square, a × a # | Any axis through the centroid | A = a² | a⁴ ÷ 12 | a³ ÷ 6 | a ÷ √12 = 0.2887a |
| Solid circle, diameter d # | Any axis through the centre | A = π·d² ÷ 4 | π·d⁴ ÷ 64 | π·d³ ÷ 32 | d ÷ 4 |
| Hollow circle, od × id # | Any axis through the centre | A = π(od² − id²) ÷ 4 | π(od⁴ − id⁴) ÷ 64 | π(od⁴ − id⁴) ÷ (32·od) | √(od² + id²) ÷ 4 |
| Hollow rectangle, b × h × t # | Uniform wall thickness t, bending about the parallel axis | A = b·h − (b−2t)(h−2t) | [b·h³ − (b−2t)(h−2t)³] ÷ 12 | [b·h³ − (b−2t)(h−2t)³] ÷ (6h) | √(Ix ÷ A) |
| I-section, idealised # | No fillets: d, flange width bf, web tw, flange tf | A = 2·bf·tf + (d−2tf)·tw | [bf·d³ − (bf−tw)(d−2tf)³] ÷ 12 | 2·Ix ÷ d | √(Ix ÷ A) |
| Triangle, base b, height h # | About the centroidal axis, parallel to the base | A = b·h ÷ 2 | b·h³ ÷ 36 | b·h² ÷ 24 | h ÷ √18 = 0.2357h |
| Thin-walled tube, mean radius r, thickness t # | Wall thickness much less than radius | A = 2π·r·t | π·r³·t | π·r²·t | r ÷ √2 = 0.7071r |
| Rectangle, about its base # | Not a centroidal axis — use for cantilever checks | A = b·h | b·h³ ÷ 3 | b·h² ÷ 3 | h ÷ √3 = 0.5774h |
Values are for the centroidal axis unless the row says otherwise — the axis through the centre of area. This matters more than anything else on the page: a rectangle about its base has I = b·h³/3, four times the centroidal value, and a beam and a cantilever are checked about different axes. S is the elastic section modulus, used for design against yield; the plastic modulus Z is 10–15% larger for an I-section and is used in plastic design. Values are for the stated shape only — holes, notches, tapers and the fillets in a real rolled section are not represented.
Every section has two principal moments of inertia, one for bending about each axis, and which one governs depends on how the member is loaded and supported.
A floor joist spanning between two walls bends about its strong axis and is checked for Ix. The same joist braced laterally against buckling is checked for Iy about the weak axis. A cantilever is also checked about the same axes but with the base condition, where I is four times the centroidal value because the neutral axis is not at mid-depth.
Getting the axis wrong by a factor of four is the classic error, and it is invisible in a calculation that otherwise looks right. State the axis on the drawing.
An I-beam or channel can be computed as the difference of rectangles using the idealised formula in the table, but the answer will be 2 to 3% low — real rolled shapes have fillets between the web and the flange, which add material exactly where it contributes most to stiffness.
That is why design values come from a published section property table rather than from geometry. Use the idealised formula here for a sanity check or an estimate, and take Ix, Sx, rx and Zx from the AISC Shapes Database or the equivalent national table for anything that will be built.
Composite and built-up sections need the parallel axis theorem on top of these formulas: I about a new axis = Icentroid + A·d², where d is the distance the axis moved. T-sections and unsymmetrical built-up beams cannot be handled by the simple formulas above.
Each data column on this page is tied to the source it came from. The numbers in square brackets correspond to the table headers above.
| # | Source | Type | Revision / method |
|---|---|---|---|
| [1] | Value computed from the standard's defining relationship | derived | Computed at build time from the defining formula stated on the page, then verified against every row and anchored by known standard values. |
| [2] | AISC Steel Construction Manual, Shapes Database | standard | AISC 15th edition (2017), Shapes Database v15.0 |
| Standard | Revision | What it covers on this page |
|---|---|---|
| AISC Steel Construction Manual, Shapes Database | AISC 15th edition (2017), Shapes Database v15.0 | the shape definitions and the axes the properties refer to |
| ASTM A6/A6M — General Requirements for Rolled Structural Steel Bars, Plates, Shapes and Sheet Piling | ASTM A6/A6M-24 | the nominal dimensions of rolled shapes |
| Roark's Formulas for Stress and Strain | Roark's, 8th edition (2011) | the closed-form section property formulas |
Cross-checked against:
Derived values — the following values on this page are calculated, not taken directly from the standard:
| Value | How it is derived |
|---|---|
| Area, I, S and r | Standard closed-form formulas for each shape, evaluated in the browser by the linked calculators and stated symbolically here. The radius of gyration entries are restatements of r = √(I/A) rather than independent values. |
Values refer to the stated axes, normally centroidal. Rolled sections need published table values because fillets add 2–3% that these idealised formulas omit. Holes, notches, tapers, composite sections and unsymmetrical built-up members are not covered — those need the parallel axis theorem or a published table.
Every value on this page is traceable to the sources listed above. If you use the data in a document, paper or report, cite it as:
Each row in the tables above also has a permanent link — hover a row and use the # link to cite a single value rather than the whole page.
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