Column buckling: Euler's formula and effective length
Why slender columns fail by bending sideways long before they crush, and how end conditions change the buckling load.
A short, stocky column fails by crushing. A long, slender one fails much earlier by buckling: it suddenly bows sideways. Euler worked out the load at which this happens.
Euler's critical load
Pcr = π² E ILe²
E is Young's modulus, I the least second moment of area (buckling happens about the weaker axis) and Le the effective length.
Effective length for different end conditions
| End conditions | Effective length Le |
|---|---|
| Both ends hinged | L |
| One end fixed, other free | 2L |
| Both ends fixed | L/2 |
| One end fixed, other hinged | L/√2 ≈ 0.7L |
Slenderness ratio
Using the least radius of gyration, k = √(I/A):
λ = Lek σcr = π² Eλ²
Euler's formula only holds when σcr is below the proportional limit. For mild steel that means λ above roughly 80 to 100. Shorter columns are designed with Rankine's or the code's formulas instead.
Worked example
A hinged–hinged steel strut, 3 m long, is a solid round bar of 50 mm diameter. E = 2 × 10⁵ N/mm².
I = π × 50⁴64 = 3.07 × 10⁵ mm⁴
Pcr = π² × 2 × 10⁵ × 3.07 × 10⁵3000² = 67.3 kN
Rankine's formula
1PR = 1Pc + 1PE
It blends crushing load Pc and Euler load PE, so it works for short and long columns alike.
Quick check
A column fixed at both ends is replaced by one hinged at both ends, same length. The Euler load becomes: