Langford Analytic · Knowledge Base

Euler Buckling Reference

Euler buckling load, critical stress, effective length factors and the Johnson-Euler transition for intermediate slenderness.

Article 03.01Buckling & Stability3 min read
Eulerbucklingcritical loadeffective lengthslendernesscolumnJohnson

Definition

Euler buckling is the elastic instability of a slender column under axial compression. The critical load is the load at which a perfectly straight column bifurcates into a bent configuration.

Equations

Euler buckling load:
         π² · E · I
P_cr  =  ───────────
           (K · L)²

Euler buckling stress:
         π² · E
σ_cr  =  ───────────
          (L'/r)²

where  L' = K · L  (effective length)
         r  =  √(I/A)  (radius of gyration)

Johnson-Euler transition (inelastic):
σ_allow  =  σ_y  −  σ_y² · (L'/r)² / (4 π² E)

Transition slenderness:
(L'/r)_trans  =  √(2 π² E / σ_y)

Effective Length Factors

End ConditionK (theoretical)K (practical)
Pinned-pinned1.01.0
Fixed-fixed0.50.65
Fixed-pinned0.70.8
Fixed-free (cantilever)2.02.1
Fixed-guided1.01.2

Variables

SymbolDefinitionUnits
P_crCritical (Euler) buckling loadN
σ_crCritical buckling stressMPa
EYoung's modulusGPa
IMinimum second moment of areamm⁴
ACross-sectional areamm²
LActual column lengthmm
KEffective length factor—
L'Effective length (K·L)mm
rRadius of gyrationmm
L'/rSlenderness ratio—
σ_yYield strengthMPa

Notes and Limitations

  • Euler buckling assumes perfect geometry, linear elasticity and concentric loading
  • Real columns have imperfections — apply a knockdown factor (typically 0.8-0.9)
  • Buckling occurs about the weak axis (minimum I) unless bracing prevents it
  • For thin-walled sections, local buckling (flange/web) may precede column buckling
  • The practical K values account for less-than-perfect end fixity

Related Knowledge

See the Structural Analysis Knowledge category for buckling theory and post-buckling behaviour. See How to Assess Column Buckling for the practical workflow.