Solid MechanicsIntermediate

Euler Column Buckling Calculator with Secant Method

Complete column buckling analysis with Euler, Johnson Parabola, and Secant methods. Calculate critical loads for eccentric loading, visualize buckling mode shapes (n=1,2,3), and explore different end conditions (K=0.5 to 2.0). Includes safety factor calculations per AISC standards.

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Column Buckling Calculator

✓ Verified Content: All equations and data verified against authoritative sources including MIT OpenCourseWare, Engineering Toolbox, and AISC Steel Construction Manual (public excerpts). See verification log

Introduction

On August 29, 1907, the Quebec Bridge (designed to be the longest cantilever span in the world) collapsed during construction, killing 75 workers. The cause? Compression chords in the main truss buckled under their own weight before the bridge was even complete. The load has to go somewhere, and when a slender column reaches its critical buckling load, "somewhere" becomes a violent sideways deflection that no amount of material strength can prevent.

This is where structures fail: not by crushing, but by suddenly bowing sideways at loads far below the material's compressive capacity. Any structural engineer will tell you: buckling is the great equalizer. A column made of the strongest steel will buckle at exactly the same load as one made of ordinary steel if they share the same geometry. First mathematically described by Leonhard Euler in 1757, buckling represents a stability failure rather than a material failure. The column doesn't run out of strength; it runs out of geometric stability.

In the real world, nothing is perfectly straight, and small initial imperfections get amplified as load approaches the critical value. This interactive column buckling calculator lets you explore how slenderness ratio, end conditions, and cross-section shape combine to determine whether your column will crush like a short, stubby post or buckle like a slender reed. This knowledge separates safe designs from future collapse investigations.

How to Use This Simulation

This interactive buckling analyzer computes critical loads, slenderness ratios, and buckling mode shapes for columns with various end conditions and cross-sections. The load has to go somewhere, and this tool shows you exactly when that load triggers the sudden sideways instability that ends a column's useful life.

Main Controls

ControlLocationFunction
End ConditionTop button rowSelect pinned-pinned (K=1), fixed-fixed (K=0.5), fixed-pinned (K=0.7), or fixed-free (K=2)
Buckling ModeMode selectorView first, second, or third buckling modes (n = 1, 2, 3)
Material PresetDropdown menuQuick-select E values for steel, aluminum, timber, or concrete
Section TypeDropdown menuChoose rectangle, circle, hollow tube, or I-beam cross-sections
Section CalculatorCollapsible panelCompute I and radius of gyration from dimensions

Input Parameters

ParameterRangeUnitsWhat It Controls
Column Length L1-10mUnsupported height between end conditions
Elastic Modulus E10-210GPaMaterial stiffness from material selection
Moment of Inertia I10-10000×10⁴ mm⁴Cross-section geometry (computed from dimensions)
Section DimensionsvariesmmWidth, height, diameter, wall thickness as applicable
Applied Load P0-2×PcrkNCurrent axial load for safety factor display

Results Display

The simulation provides comprehensive buckling analysis:

  • Buckling Animation: Visual representation of the buckled mode shape. First mode is a single half-wave; higher modes show multiple waves.
  • Critical Load Pcr: The Euler buckling load in kN. This is where structures fail, suddenly and without warning when this value is reached.
  • Critical Stress σcr: Buckling load divided by area (MPa). Compare to yield strength to determine failure mode.
  • Slenderness Ratio λ: KL/r value that classifies columns as short, intermediate, or long.
  • Classification: Indicates whether column will fail by crushing (short), inelastic buckling (intermediate), or elastic Euler buckling (long).
  • Safety Factor: Ratio of critical load to applied load. Any structural engineer will tell you that factors of 2.5-3 are typical for columns.

Tips for Exploration

  1. Watch the K-factor effect. Switch from fixed-fixed (K=0.5) to fixed-free (K=2) with the same length and cross-section. The critical load drops by a factor of 16 (that's K² in the denominator). This is where structures fail when designers assume rigid connections that are actually loose or flexible.

  2. Find the slenderness transition. Start with a long, slender column and gradually increase the cross-section size. Watch the classification change from "Long (Euler)" to "Intermediate" to "Short." Each regime requires different design equations, and mixing them up leads to unconservative designs.

  3. Compare solid vs. hollow sections. Set up a solid circular column, note the critical load, then switch to a hollow tube with the same outer diameter. The hollow section has higher I per unit area, making it more efficient against buckling. Any structural engineer will tell you that this is why structural tubes are preferred for compression members.

  4. Explore higher buckling modes. Click through n = 1, 2, 3 to see how critical load increases with mode number (Pcr ∝ n²). In practice, first mode governs unless intermediate bracing prevents it. When you add a midpoint brace, you're essentially forcing the column into a higher mode.

  5. Test material sensitivity. The load has to go somewhere, but Euler buckling doesn't care about material strength, only stiffness. Double the modulus E and watch the critical load double. A slender steel column buckles at the same load as a slender aluminum column of identical geometry, not because aluminum is weaker in compression (it is), but because its modulus is lower (E = 69 GPa vs. 200 GPa).

What Is Column Buckling?

Column buckling is a stability failure phenomenon where a slender structural member under axial compression suddenly deflects laterally at a critical load, well before the material's compressive strength is reached [1]. First derived mathematically by Swiss mathematician Leonhard Euler in 1757, the critical buckling load Pcr depends on the column's flexural stiffness (EI), length (L), and end support conditions (K-factor) [2].

The fundamental equation: Pcr = π²EI / (KL)²

Unlike crushing or yielding, buckling is geometrically driven: the column loses stability rather than material strength. This makes it particularly dangerous because the transition from stable to unstable is sudden and catastrophic, with little warning deflection before collapse [3].

Types of End Conditions and K-Factors

The way a column's ends are supported dramatically affects its buckling resistance through the effective length factor (K) [4]. Different end conditions create different buckling mode shapes and effective lengths:

1. Pinned-Pinned (K = 1.0)

  • Description: Both ends are free to rotate but cannot translate laterally. This is the theoretical baseline condition used in Euler's original derivation.
  • Real-World Examples: Simple truss members, temporary scaffolding, bridge compression members with pin connections, laboratory test specimens
  • Buckling Mode: Single half-sine wave with inflection points at both ends
  • Effective Length: Le = L (the entire length buckles)

2. Fixed-Fixed (K = 0.5)

  • Description: Both ends are prevented from rotating and translating. This provides the maximum buckling resistance.
  • Real-World Examples: Building columns with moment-resisting connections at floor slabs, vertical members in rigid steel frames, compression members in welded structures
  • Buckling Mode: Reverse-curvature S-shape with inflection points at quarter-length positions
  • Effective Length: Le = 0.5L (only the middle half buckles, providing 4× the strength of pinned-pinned)

3. Fixed-Pinned (K = 0.7)

  • Description: One end is fixed (rotation prevented), the other is pinned (free to rotate).
  • Real-World Examples: Building columns fixed at foundation but pinned at roof level, bridge piers fixed at base, mast structures
  • Buckling Mode: Asymmetric curve with inflection point closer to the pinned end
  • Effective Length: Le = 0.7L (approximately 2× stronger than pinned-pinned)

4. Fixed-Free (K = 2.0)

  • Description: One end is completely fixed, the other is free (cantilevered). This is the weakest configuration.
  • Real-World Examples: Flagpoles, cantilever sign posts, antenna masts, vertical elements of cantilever structures, crane booms
  • Buckling Mode: Quarter-sine wave with maximum deflection at the free end
  • Effective Length: Le = 2.0L (effectively twice as long, providing only 1/4 the strength of pinned-pinned)

Key Parameters in Buckling Analysis

ParameterSymbolUnitsTypical RangePhysical Meaning
Critical Buckling LoadPcrkN10-10,000 kNMaximum axial load before buckling occurs
Young's ModulusEGPa10-210 GPaMaterial stiffness (steel: 200, aluminum: 69, timber: 12)
Moment of InertiaImm⁴ × 10⁶0.1-1000Cross-section's resistance to bending (always use minimum I)
Column LengthLm1-20 mActual physical length between supports
Effective LengthLem0.5L-2.0LBuckling length accounting for end conditions (Le = KL)
K-FactorK-0.5-2.0Effective length factor based on end restraint
Cross-Sectional AreaAmm²1,000-100,000Total area resisting axial stress
Radius of Gyrationrmm10-200 mmr = √(I/A), measure of section compactness
Slenderness Ratioλ-10-300λ = Le/r, indicates buckling vs crushing behavior
Critical StressσcrMPa1-250 MPaAverage stress at buckling (Pcr/A)
Safety FactorFS-1.67-3.0Design margin (typical: 2.0 for buildings, 3.0 for aerospace)

Essential Formulas

Euler Critical Load (Long Columns)

Pcr = π²EI / Le²

Le = KL

Where:

  • Pcr = Critical buckling load (kN)
  • π = 3.14159...
  • E = Young's modulus (GPa)
  • I = Second moment of area about the weak axis (mm⁴ × 10⁶)
  • Le = Effective length (m)
  • K = Effective length factor (0.5 to 2.0)
  • L = Actual column length (m)

Key Insight: Pcr is inversely proportional to Le². Doubling the length reduces buckling strength by 4×. Halving the K-factor (fixed-fixed vs pinned-pinned) increases strength by 4×.

Radius of Gyration and Slenderness Ratio

r = √(I / A)

λ = Le / r

The slenderness ratio λ determines column behavior:

  • λ < 50: Short column, failure by crushing (use material strength)
  • 50 < λ < Cc: Intermediate column, use Johnson parabola formula
  • λ > Cc: Long column, use Euler formula (buckling dominates)

Critical Slenderness Ratio (Transition Point)

Cc = π√(2E / Fy)

Where Fy is the yield strength (MPa). For steel (E=200 GPa, Fy=250 MPa): Cc ≈ 126

Johnson Parabola (Intermediate Columns)

σcr = Fy - (Fy²λ²) / (4π²E)

This empirical formula bridges the gap between crushing and buckling failure for intermediate slenderness ratios.

Design Allowable Load

Pallow = Pcr / FS

Typical safety factors:

  • Building structures: FS = 1.67-2.0
  • Bridges: FS = 2.0-2.5
  • Aerospace: FS = 1.5-3.0 (depending on criticality)
  • Crane structures: FS = 2.0-3.0

Learning Objectives

After exploring this simulation, you will be able to:

  1. Calculate critical buckling loads for columns with different end conditions using Euler's formula and understand how the K-factor affects buckling resistance
  2. Determine slenderness ratios and classify columns as short, intermediate, or long based on the transition slenderness ratio Cc
  3. Visualize buckling mode shapes for different end conditions and understand how higher buckling modes (n=2, n=3) occur at higher loads
  4. Compare effective lengths for different support configurations and explain why fixed-fixed columns are 4× stronger than pinned-pinned columns of the same dimensions
  5. Select appropriate cross-sections by calculating moment of inertia and radius of gyration for rectangles, circles, pipes, and I-beams
  6. Apply safety factors to determine allowable design loads and assess whether actual applied loads are within safe limits

Exploration Activities

Activity 1: Effect of End Conditions on Buckling Strength

Objective: Compare how different support conditions affect the same column's buckling resistance

Steps:

  1. Set up a baseline column: E = 200 GPa, L = 5m, rectangle 100×200mm (I = 66.67×10⁶ mm⁴, A = 20,000 mm²)
  2. Select "Pinned-Pinned" and record the critical load Pcr
  3. Switch to "Fixed-Fixed" and compare the new Pcr
  4. Try "Fixed-Pinned" and "Fixed-Free" and record all results
  5. Calculate the ratio of Pcr(fixed-fixed) to Pcr(pinned-pinned)

Observe: Fixed-Fixed provides exactly 4× the buckling strength of Pinned-Pinned because K is halved (from 1.0 to 0.5) and Pcr ∝ 1/K²

Expected Result: For the baseline column: Pinned-Pinned ≈ 526 kN, Fixed-Fixed ≈ 2,104 kN, Fixed-Pinned ≈ 1,074 kN, Fixed-Free ≈ 131 kN

Activity 2: Length² Relationship

Objective: Verify that buckling load is inversely proportional to the square of length

Steps:

  1. Set Pinned-Pinned, E = 200 GPa, I = 50×10⁶ mm⁴, A = 10,000 mm²
  2. Set L = 2m and record Pcr
  3. Double the length to L = 4m and record new Pcr
  4. Try L = 8m
  5. Calculate the ratios Pcr(2m)/Pcr(4m) and Pcr(4m)/Pcr(8m)

Observe: Each doubling of length reduces Pcr by a factor of 4 (not 2), confirming the L² relationship

Expected Result: Pcr(2m) = 2,467 kN, Pcr(4m) = 617 kN (ratio ≈ 4), Pcr(8m) = 154 kN (ratio ≈ 4)

Activity 3: Slenderness Transition and Column Classification

Objective: Understand the transition from short to long column behavior

Steps:

  1. Select material preset "Structural Steel" (E = 200 GPa, Fy = 250 MPa)
  2. Calculate Cc: Cc = π√(2E/Fy) = π√(400,000/250) ≈ 126
  3. Set up a column with λ = 50 (short): L = 2m, rectangle 100×200mm (r ≈ 57.7mm, need Le = 2.89m, so use L ≈ 2.9m with K=1)
  4. Increase length to get λ = 100 (intermediate): L ≈ 5.8m
  5. Increase further to get λ = 150 (long): L ≈ 8.7m
  6. Observe the classification change and how the current point moves through the chart's Euler and Johnson regions

Observe: Below Cc, the Johnson parabola (amber curve) applies; above Cc, the Euler curve (blue) applies

Activity 4: Higher Buckling Modes

Objective: Explore how columns can buckle in higher mode shapes at increased loads

Steps:

  1. Set Pinned-Pinned, E = 200 GPa, L = 6m, I = 100×10⁶ mm⁴
  2. Select buckling mode n = 1 and record Pcr
  3. Switch to mode n = 2 and observe the buckling shape and new Pcr
  4. Try mode n = 3
  5. Calculate the ratios Pcr(n=2)/Pcr(n=1) and Pcr(n=3)/Pcr(n=1)

Observe: Higher modes have more waves and buckle at loads proportional to n² (mode 2 at 4× load, mode 3 at 9× load)

Real-World Applications

  • Building Columns: Multi-story buildings use W-shape steel columns (I-beams) or HSS (hollow structural sections) as vertical load-bearing members. A typical 4-story building column might be W250×73 (I ≈ 90×10⁶ mm⁴) with height 4m per floor and fixed-pinned conditions (K=0.7), requiring buckling checks for each story.

  • Bridge Piers and Towers: Highway bridge piers supporting long spans act as compression columns subject to dead loads, live loads, wind, and seismic forces. The iconic Golden Gate Bridge has towers 227m tall acting as cantilever columns at the top but with intermediate bracing that reduces effective length.

  • Aerospace Structures: Aircraft fuselage frames, wing ribs, and landing gear struts are critical compression members where weight savings drive the use of high-strength aluminum (7075-T6, E=72 GPa, Fy=500 MPa) or titanium alloys.

  • Flagpoles and Antenna Masts: Tall flagpoles (8-30m) are classic fixed-free cantilever columns (K=2.0) subject to wind loading.

  • Scaffolding and Temporary Structures: Construction scaffolding uses tubular steel members (typically 48mm OD) in compression. OSHA requires that scaffold leg loads be checked for buckling with appropriate K-factors.

  • Mechanical Linkages and Actuators: Hydraulic cylinders, push rods in engines, and robotic actuators operate as compression members.

  • Truss Compression Chords: Top chords of roof trusses and bottom chords of bridge trusses carry compression with bracing providing K ≈ 0.8.

Reference Data Tables

Effective Length Factors (K) for Common Configurations

End ConditionK-FactorTheoreticalDesign Code ValueCommon Applications
Fixed-Fixed0.50.50.65*Building columns with rigid connections both ends
Fixed-Pinned0.70.6990.80*Columns fixed at base, pinned at top
Pinned-Pinned1.01.01.0Truss members, simple connections
Fixed-Free2.02.02.1*Flagpoles, cantilever columns
Fixed-Guided1.01.01.2*Columns in braced frames
Fixed-Fixed (sidesway)1.01.01.0Unbraced frames (sidesway permitted)

Design codes (AISC, Eurocode) use conservative values accounting for real-world imperfections

Material Properties for Buckling Analysis

MaterialE (GPa)Fy (MPa)Cc (approx.)Density (kg/m³)Notes
Structural Steel A362002501267850Most common construction steel
High-Strength Steel A9922003451077850Modern wide-flange shapes
Stainless Steel 3041932151348000Corrosion resistance
Aluminum 6061-T669240762700Good strength-to-weight
Aluminum 7075-T672500532810Aerospace applications
Titanium Ti-6Al-4V114880514430High performance, expensive
Southern Pine (timber)123089550Parallel to grain
Douglas Fir (timber)133586530Structural lumber
Concrete (normal)25301292400Compressive strength Fc, not Fy
Carbon Fiber Composite150600711600Highly anisotropic, directional

Typical Cross-Section Properties

Section TypeDimensionsA (mm²)I (×10⁶ mm⁴)r (mm)Efficient Use
W250×73 I-beambf=254, tf=14.2, hw=222, tw=8.6928089.598.2Building columns
HSS 200×200×10Square tube 200×200, t=10744049.981.9Architectural columns
Pipe 150mm Sch 40OD=168.3, t=7.136508.548.3Moderate loads
Rectangle 100×200Solid rectangle20,00066.757.7Timber posts, concrete
Circle 150mmSolid circular17,67124.937.5Simple round columns

Challenge Questions

  1. Conceptual: Why does the Euler formula not depend on the material's yield strength (Fy), yet crushing failure does? At what slenderness ratio does this transition occur for steel (E=200 GPa, Fy=250 MPa)?

  2. Calculation: A 6m tall steel column (E=200 GPa) with W200×46 section (I=45.5×10⁶ mm⁴, A=5890 mm²) has fixed-pinned end conditions. Calculate: (a) effective length Le, (b) radius of gyration r, (c) slenderness ratio λ, (d) critical load Pcr, (e) allowable load with FS=2.0

  3. Analysis: Two columns have the same material, length, and cross-sectional area, but Column A is pinned-pinned and Column B is fixed-fixed. If Column A fails at 500 kN, at what load will Column B fail? Explain using the K-factor relationship.

  4. Application: You are designing a 10m tall flagpole (fixed-free, K=2.0) to support a lateral wind load equivalent to 50 kN axial compression. Using aluminum 6061 (E=69 GPa), what minimum diameter circular tube with 5mm wall thickness is required with FS=2.5?

  5. Design: A building column must carry 2000 kN. It is 4m tall with fixed-pinned conditions. Compare three options: (1) W250×73 steel (I=89.5×10⁶, A=9280), (2) HSS 200×200×10 (I=49.9×10⁶, A=7440), (3) Solid rectangle 150×300mm (I=337.5×10⁶, A=45,000). Which is most efficient by weight?

  6. Comparison: A compression member in a truss has L=3m between pin joints. If you add a lateral brace at midpoint (preventing deflection there), how does this change the effective length and critical load? (Hint: the brace creates two columns in series)

Common Mistakes to Avoid

In the real world, nothing is perfectly straight, and these calculation errors make the difference between columns that stand and columns that collapse:

  • Using the wrong axis moment of inertia: This is where structures fail. Columns buckle about the weak axis (minimum I). For a rectangle 100×200mm standing vertically, the weak axis is about the 100mm width, giving I = 100×200³/12 = 66.7×10⁶ mm⁴, NOT I = 200×100³/12 = 16.7×10⁶ mm⁴. Always use Imin unless lateral bracing prevents buckling about one axis.

  • Forgetting to apply the K-factor: Using L instead of Le = KL in the Euler formula overestimates buckling strength by 1/K². For a fixed-fixed column (K=0.5), using L instead of 0.5L overestimates Pcr by 4x, a potentially catastrophic error. Always identify end conditions and apply the correct K-factor.

  • Applying Euler's formula to short columns: Euler's formula only applies when λ > Cc (long columns). For λ < Cc, use the Johnson parabola or design for crushing strength. A stocky column with λ = 30 will crush at σ = Fy before it buckles; using Euler's formula would predict an impossibly high Pcr > Fy × A.

  • Ignoring load eccentricity: Real columns rarely have perfectly centered loads. Even small eccentricity (e) creates bending moment M = P×e, reducing capacity via the secant formula. Design codes use interaction equations like P/Pn + M/Mn ≤ 1.0 to account for combined axial-plus-bending.

  • Confusing slenderness ratio (λ = Le/r) with aspect ratio (L/d): Slenderness ratio uses radius of gyration r = √(I/A), not diameter or width. Two columns with the same L/d can have vastly different λ values if their cross-sections differ (hollow vs solid). Always calculate r properly from the section's I and A.

Frequently Asked Questions

Why doesn't the Euler formula include material yield strength?

Euler's formula (Pcr = π²EI/Le²) only involves Young's modulus (E) because buckling is a geometric stability phenomenon, not a material strength failure [1]. The column deflects sideways at Pcr regardless of how strong the material is. Yield strength only matters when the buckling stress exceeds Fy, which happens in short, stocky columns where λ < Cc. That's why we need both Euler's formula (for long columns) and the Johnson parabola (for intermediate columns) to cover all cases [5].

How do I know if my column is "long" or "short"?

Calculate the slenderness ratio λ = Le/r and compare it to the critical slenderness Cc = π√(2E/Fy) [2]. For structural steel (E=200 GPa, Fy=250 MPa), Cc ≈ 126. If λ > Cc, it's a long column (Euler formula applies). If λ < Cc, use the Johnson parabola for intermediate columns [5]. If λ < 50, the column is so stocky it will crush before buckling. Use material compressive strength instead.

Why is fixed-fixed 4× stronger than pinned-pinned for the same column?

Because Pcr ∝ 1/Le² and Le = KL [4]. For fixed-fixed, K = 0.5, so Le = 0.5L. For pinned-pinned, K = 1.0, so Le = L. The ratio of buckling loads is (1/0.5²)/(1/1²) = 4. Physically, the fixed ends create inflection points at L/4 from each end, so only the middle half of the column effectively buckles [3].

What happens if I apply load eccentrically (off-center)?

Eccentric loading creates combined axial compression plus bending moment (M = P × e, where e is eccentricity) [6]. This significantly reduces capacity because the column must resist both effects. The secant formula accounts for this: σmax = P/A × [1 + (ec/r²)sec(Le/(2r)√(P/AE))]. Even small eccentricities (e.g., 25mm on a 200mm column) can reduce allowable load by 30-50% [7].

Can I increase buckling resistance without changing the column size?

Yes, several strategies work [3]: (1) Add lateral bracing at mid-height to reduce effective length. A brace at midpoint cuts Le in half and increases Pcr by 4x. (2) Change end conditions. Converting pinned-pinned to fixed-pinned increases capacity by about 2x. (3) Use a hollow section instead of solid. A pipe has much higher I than a solid circle of the same area because material is farther from the centroid.

References

  1. MIT OpenCourseWare 2.080J: Structural Mechanics lecture notes on column buckling and stability. Available at: https://ocw.mit.edu/courses/2-080j-structural-mechanics-fall-2013/ (CC BY-NC-SA)

  2. Engineering Toolbox - Column Buckling: Comprehensive resource on Euler's formula, effective length factors, and buckling calculations. Available at: https://www.engineeringtoolbox.com/euler-column-formula-d_1813.html (Free educational resource)

  3. NPTEL Structural Analysis: Indian Institute of Technology lectures on buckling and stability of compression members. Available at: https://nptel.ac.in/courses/105106116 (Free educational resource)

  4. AISC 360 Commentary (Public): Commentary on effective length factors and column stability concepts. Available at: https://www.aisc.org/publications/steel-standards/ (Public excerpts available)

  5. HyperPhysics - Buckling: Georgia State University physics resource explaining Euler buckling fundamentals. Available at: http://hyperphysics.gsu.edu/hbase/permot2.html (Free educational resource)

  6. Continuum Mechanics - Column Buckling: Physical derivation of Euler buckling theory with emphasis on understanding the mechanics. Available at: https://www.continuummechanics.org/columnbuckling.html (Free educational resource)

  7. LibreTexts Engineering: Open-access mechanics of materials textbook covering column buckling and design. Available at: https://eng.libretexts.org/Bookshelves/Mechanical_Engineering (CC BY)

  8. Khan Academy - Structural Engineering: Foundation concepts on stress, strain, and structural stability. Available at: https://www.khanacademy.org/science/physics (Free educational resource)

About the Data

Material property data (Young's modulus, yield strength) used in this simulation are based on standard engineering references including the Engineering Toolbox database and AISC Steel Manual public excerpts. K-factors for end conditions follow the theoretical values derived by Euler and subsequent researchers, with design values referencing AISC 360 commentary. All formulas use the internationally recognized Euler-based approach for slender columns and the Johnson parabola for intermediate columns.

How to Cite

Simulations4All Team. "Column Buckling Calculator: Understanding Euler's Critical Load." Simulations4All, 2025. Available at: https://simulations4all.com/simulations/column-buckling

Verification Log

Claim/DataSourceStatusDate
Euler formula: Pcr = π²EI/Le²MIT OCW 2.080J, Engineering Toolbox [1, 2]✓ VerifiedDec 2025
K-factors: 0.5 (fixed-fixed), 0.7 (fixed-pinned), 1.0 (pinned-pinned), 2.0 (fixed-free)AISC 360 Commentary, Engineering Toolbox [2, 4]✓ VerifiedDec 2025
Critical slenderness Cc = π√(2E/Fy)MIT OCW, HyperPhysics [1, 5]✓ VerifiedDec 2025
Johnson parabola for intermediate columnsEngineering Toolbox, LibreTexts [2, 7]✓ VerifiedDec 2025
Steel A36 properties: E=200 GPa, Fy=250 MPaEngineering Toolbox, AISC public data [2, 4]✓ VerifiedDec 2025
Aluminum 6061-T6: E=69 GPa, Fy=240 MPaEngineering Toolbox, MatWeb public data [2]✓ VerifiedDec 2025
Moment of inertia formulas for rectangle, circle, pipe, I-beamNPTEL, LibreTexts [3, 7]✓ VerifiedDec 2025
Radius of gyration r = √(I/A)MIT OCW, HyperPhysics [1, 5]✓ VerifiedDec 2025

Written by Simulations4All Team

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