Columns and Buckling
The one failure mode that is not about strength at all. Euler's formula contains no yield stress, which is why a stronger steel buys you nothing.
Skip to the animationBuckling is a stability failure rather than a strength failure: a slender column collapses sideways at P_cr = π²EI/Lₑ², a load that depends on stiffness and geometry and contains no yield stress at all — which is why a stronger steel buys no extra capacity.
A different kind of failure
A short block in compression crushes when the stress reaches yield. A slender strut never gets there: it bows sideways and collapses at a stress the material could carry comfortably.
The question changes form too. Not "is the stress acceptable" but "what happens after a small disturbance" — does the strut return to straight, or does the bow grow? That is a stability question, and it needs its own analysis.
Euler's critical load
- 1Below the critical load, a sideways disturbance is resisted and the strut springs back. Stable.
- 2At the critical load, straight and slightly bent require the same load. The strut is indifferent.
- 3Above it, any disturbance grows rather than decaying, and collapse follows.
- 4Solving the resulting differential equation gives P_cr = π²EI/Lₑ².
Look at what the formula does not contain: the yield stress. All structural steels have E ≈ 200 GPa regardless of grade, so specifying high-strength steel for a slender column buys nothing at all. The gain has to come from I or from a shorter effective length.
Effective length
| End conditions | Effective length Lₑ | Relative capacity |
|---|---|---|
| Both ends pinned | L | 1.0 — the reference case |
| Both ends fixed | 0.5 L | 4.0 |
| One fixed, one pinned | 0.7 L | ≈ 2.0 |
| Fixed at the base, free at the top | 2 L | 0.25 |
Since P_cr ∝ 1/Lₑ², the range from fixed-fixed to fixed-free spans a factor of sixteen for the same strut, the same material and the same section.
The practical caution is that real connections are semi-rigid. A bolted end plate is neither pinned nor fixed, and claiming full fixity from a joint that cannot deliver it is unconservative in a failure mode that gives no warning.
The weakest axis governs
A column buckles about the axis with the smallest I — never the one you were designing for. An I-section is excellent in bending about its strong axis and a poor column unless its weak axis is braced.
A circular hollow section has the same I in every direction, which is why it is the natural choice for a free-standing column. Bracing exists precisely to shorten the effective length about the weak axis, and it is why a slender column with mid-height restraint carries four times as much.
Where Euler's formula is wrong
Extrapolated to a short column, Euler's formula predicts a buckling stress above the yield stress — which the material cannot reach, so it crushes first. The formula is valid only above a critical slenderness ratio.
- Rankine's formula blends the crushing and buckling regimes into one expression.
- Design codes use curves fitted to test data, with separate curves for different section types and manufacturing routes.
- Slenderness ratio
Lₑ/kis the parameter that decides which regime a column is in, where k is the radius of gyration.
Why real columns are weaker still
| Imperfection | Effect |
|---|---|
| Initial crookedness | No rolled section is perfectly straight; the bow starts before the load arrives |
| Load eccentricity | Never applied exactly on the axis, so a moment exists from the start |
| Residual stresses | Left by rolling and welding; parts of the section yield early |
| Accidental lateral load | Wind, impact, construction tolerance |
All of them push the same way, so measured capacities sit consistently below the theoretical curve. Buckling also gives no warning — no yielding, no cracking, no visible sag — which is why column safety factors are the largest in the subject.
The numbers you will be asked for
- Euler critical load
P_cr = π²EI / Lₑ²
- Critical stress
σ_cr = π²E / (Lₑ/k)²
- Radius of gyration
k = √(I / A)
- Slenderness ratio
λ = Lₑ / k
- Rankine's formula
P = σc·A / (1 + a·λ²)
blends crushing and buckling
Watch it work
Check yourself
question 1 / 4
One question at a time. Pick an answer to see why it is right or wrong, then move on — there is no score to keep and nothing is saved.