The formulas
| Pe | = π² E I(K L)² | Euler buckling load |
|---|---|---|
| r | = √(I / A) | radius of gyration |
| Fe | = π² E(K L / r)² | Euler buckling stress |
| Cc | = √(2π² E / Fy) | where Fe = Fy / 2 |
| Fcr | = Fy [1 − (KL/r)² / (2Cc²)] | Johnson, KL/r < Cc |
| Fcr | = 0.658Fy/Fe Fy | AISC, Fy/Fe ≤ 2.25 |
| Fcr | = 0.877 Fe | AISC, Fy/Fe > 2.25 |
Effective length factors
| Ends | Theoretical K | Recommended K |
|---|---|---|
| Pinned at both ends | 1.0 | 1.0 |
| Fixed base, pinned top | 0.7 | 0.8 |
| Fixed at both ends | 0.5 | 0.65 |
| Fixed base, free top (flagpole) | 2.0 | 2.1 |
| Fixed at both ends, top free to sway | 1.0 | 1.2 |
Worked example: W8×31, 14 ft, pinned ends
About the weak axis, I = 37.1 in⁴ and A = 9.13 in², so r = 2.016 in and KL/r = 168 / 2.016 = 83.3. Euler gives Fe = π² × 29,000 / 83.3² = 41.2 ksi and Pe = 376 kips. That is less than Cc = 107, so the column is in the inelastic range: Johnson gives 34.8 ksi. With Fy = 50 ksi, AISC gives Fcr = 0.65850/41.2 × 50 = 30.1 ksi, Pn = 275 kips and φPn = 247 kips. The AISC Manual's column table lists about 248 kips for this shape and length.
Questions
Why is the Euler load higher than the AISC strength?
Euler assumes a perfectly straight, perfectly elastic column. Real columns are slightly crooked and have residual stresses from rolling and welding, so they fail sooner, especially at middle slenderness. The AISC curve is fitted to tests of real columns.
Which moment of inertia should I use?
The column buckles about the axis with the larger KL/r. If it is braced differently about each axis, check both and use the larger slenderness.
Does this work for wood or aluminum?
The Euler and Johnson results work for any material with the right E and yield stress. The AISC rows are for steel only. Wood columns are designed with the NDS column stability factor, which the WebStructural column designer handles.