INGENIA

CIV-01

Euler buckling load

Critical compressive load of a slender elastic column.

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StabilityEuler 1744EN 1993-1-1

Governing equation

Pcr=π2EI(KL)2P_{\mathrm{cr}} = \dfrac{\pi^2 E I}{(K L)^2}

L∈[0.5,20]L \in \left[0.5, 20\right]

where

E
Young modulus (GPa)
I
Second moment (cm⁴)
L
Length (m)
K
Effective-length factor (—)
P_{\mathrm{cr}}
Euler load (kN)

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CIV-01 · beam
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①

Governing law — red

Pcr=π2EI(KL)2P_{\mathrm{cr}} = \dfrac{\pi^2 E I}{(K L)^2}

L∈[0.5,20]L \in \left[0.5, 20\right]

L=0.5L = 0.5Pcr=6.32×105P_{\mathrm{cr}} = 6.32\times 10^{5}

②

Domain of the variable — blue

Lmin⁡=0.5,Lmax⁡=20L_{\min} = 0.5,\quad L_{\max} = 20

L∈[0.5,20]L \in \left[0.5, 20\right]

L=0.5L = 0.5L=0.5L = 0.5

③

Response curve — green

Pcr=π2EI(KL)2P_{\mathrm{cr}} = \dfrac{\pi^2 E I}{(K L)^2}

L∈[0.5,20]L \in \left[0.5, 20\right]

L=0.5L = 0.5Pcr=6.32×105P_{\mathrm{cr}} = 6.32\times 10^{5}

④

Rate of change — amber

dPcrdL\frac{\mathrm{d}P_{\mathrm{cr}}}{\mathrm{d}L}

L∈[0.5,20]L \in \left[0.5, 20\right]

L=0.623L = 0.623Pcr′=−1.42×106P_{\mathrm{cr}}^{\prime} = -1.42\times 10^{6}

Lecture brief

Historical brief

From Euler’s 1744 elastica and Navier’s beam theory to Mohr’s circle and transformed-section RC, structural mechanics grew as a closed-form craft before finite elements. The lab keeps those governing lines for buckling, flexure, joints and influence. This sheet (CIV-01 — Euler buckling load) is the form associated with Euler 1744 · EN 1993-1-1. Working symbols: EE, II, LL, KK →\rightarrow PcrP_{\mathrm{cr}}. Euler solved the elastica eigenvalue problem Pcr = π² EI /(KL)². The effective-length factor K encodes end restraint.

Purpose

Purpose: compute PcrP_{\mathrm{cr}} from EE, II, LL, KK in Structural & civil via Pcr=π2EI(KL)2P_{\mathrm{cr}} = \dfrac{\pi^2 E I}{(K L)^2} Critical compressive load of a slender elastic column. Use it when a real structural & civil question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given E=200.000 GPaE = 200.000\,\mathrm{GPa}, I=8000.000 cm4I = 8000.000\,\mathrm{cm⁴}, L=4.000 mL = 4.000\,\mathrm{m}, K=1.000 —K = 1.000\,\mathrm{—}, the governing relation Pcr=π2EI(KL)2P_{\mathrm{cr}} = \dfrac{\pi^2 E I}{(K L)^2} yields Pcr=9869.604 kNP_{\mathrm{cr}} = 9869.604\,\mathrm{kN}. Prismatic, initially straight, concentric load, remains elastic. Move a slider: the numbers are this situation, not a canned story.

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Outputs

  • Euler load P_{\mathrm{cr}}9869.604 kN
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CIV-01 · beam
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Narration of this film

Prismatic, initially straight, concentric load, remains elastic.

Euler solved the elastica eigenvalue problem Pcr = π² EI /(KL)². The effective-length factor K encodes end restraint.

Reading speed

Watch on YouTube