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Natural Frequency of Beam Calculator – Vibration Analysis (Steel & Wood)

Natural Frequency of Beam Calculator - Compute resonant frequencies for structural beams with Euler-Bernoulli and Timoshenko theories.
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The Natural Frequency of Beam Calculator evaluates vibration and dynamic serviceability for steel and wood beams. Calculate fundamental natural frequency (fn in Hz) across simple, cantilever, fixed, and continuous supports.

Input section properties, span, and mass — receive frequency results, angular frequency, and practical guidance against human comfort limits (e.g., floor vibration 4–5 Hz).

Essential for floor systems, bridges, or sensitive structures. Complements static checks from our Ultimate Steel Beam Calculator.

Natural Frequency of Beam Calculator

Euler-Bernoulli & Timoshenko Theory  ·  Multi-Mode Analysis  ·  Resonance Checker

Euler-Bernoulli Timoshenko Multi-Mode SI / Imperial PDF Export
⚙ Unit System:
Boundary Conditions & Theory
β1L = π (3.14159)
Use Timoshenko when L/h < 10
Beam Geometry
m
m
m
Material Properties
GPa
kg/m\u00B3
kg
Added concentrated mass at beam center
Typical: steel 0.01-0.02 | concrete 0.05
N
Hz
Resonance check: warns if within ±15% of natural freq
Accuracy Note: Results are based on classical Euler-Bernoulli or Timoshenko beam theory for uniform, prismatic beams. Real structures may differ due to joint stiffness, shear-lag, material inhomogeneity, and support conditions. Always verify with FEA for critical designs. Errors exceeding 5% may occur for L/h < 5 with Euler-Bernoulli theory.
No calculation yet
Fill in the inputs and click Calculate to see results.
--
Fundamental Frequency f₁ Hz
--
Angular Frequency ω₁ rad/s
--
Period T s
--
Damped Freq. fd Hz
Computed Section Properties
Multi-Mode Frequency Table
Mode n βnL fn (Hz) ωn (rad/s) Tn (s) fd,n (Hz) Resonance Risk
Core Formula — Euler-Bernoulli Theory

For a uniform prismatic beam, the natural frequency of the n-th mode is:

Fundamental / nth Mode Frequency
\[ f_n = \frac{(\beta_n L)^2}{2\pi L^2} \sqrt{\frac{EI}{\rho A}} \]

Equivalently in angular form: \(\omega_n = \frac{(\beta_n L)^2}{L^2} \sqrt{\frac{EI}{\rho A}}\)

Where:
  • \(f_n\) = natural frequency of mode n (Hz)
  • \(\beta_n L\) = eigenvalue / frequency constant (depends on BC and mode)
  • \(E\) = Young's modulus (Pa)
  • \(I\) = second moment of area (m\u2074)
  • \(\rho\) = material density (kg/m\u00B3)
  • \(A\) = cross-sectional area (m\u00B2)
  • \(L\) = beam length (m)
Eigenvalues \(\beta_n L\) by Boundary Condition
BCMode 1Mode 2Mode 3Mode 4Mode 5
Simply Supported (SS)\(\pi\)\(2\pi\)\(3\pi\)\(4\pi\)\(5\pi\)
Cantilever (CF)1.87514.69417.854810.995514.1372
Fixed-Fixed (CC)4.73007.853210.995614.137217.2788
Fixed-Pinned (CP)3.92667.068610.210213.351816.4934
Free-Free (FF)4.73007.853210.995614.137217.2788

For SS: \(\beta_n L = n\pi\). For CF and others, values are roots of the characteristic equation.

Section Moment of Inertia Formulas
Rectangular (b × h)
\[ I = \frac{b \, h^3}{12} \qquad A = b \cdot h \]
Circular Solid (diameter d)
\[ I = \frac{\pi d^4}{64} \qquad A = \frac{\pi d^2}{4} \]
Hollow Pipe (OD, ID)
\[ I = \frac{\pi (OD^4 - ID^4)}{64} \qquad A = \frac{\pi (OD^2 - ID^2)}{4} \]
I-Beam (flanges + web)
\[ I = \frac{b_f \, h_{total}^3 - (b_f - t_w) h_w^3}{12} \]
Damped Natural Frequency
Damped Frequency
\[ f_d = f_n \sqrt{1 - \zeta^2} \]

where \(\zeta\) = damping ratio (0 for undamped, 1 for critically damped)

Axial Load Effect (Euler-Bernoulli)
Modified Frequency with Axial Load
\[ f_{n,P} = f_n \sqrt{1 + \frac{P}{P_{cr,n}}} \] \[ P_{cr,n} = \frac{(\beta_n L)^2 \, EI}{L^2} \]

P > 0: tension (increases \(f_n\)); P < 0: compression (decreases \(f_n\)). Critical buckling when P = \(-P_{cr}\).

Timoshenko Beam Correction
Timoshenko Frequency Ratio
\[ \frac{\omega_{Tim}}{\omega_{EB}} = \frac{1}{\sqrt{1 + (\beta_n r)^2 \left(\frac{E}{\kappa G} + 1\right)}} \]

r = radius of gyration = \(\sqrt{I/A}\); \(\kappa\) = shear correction factor; G = shear modulus

Mode Shape Diagram

Schematic mode shapes for first 3 modes. Select a boundary condition to update the diagram.

Calculate first to see mode shapes

Dashed centerline indicates beam neutral axis; curve shows approximate deflection shape.

Boundary Condition Schematics
✓ Copied to clipboard!

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Natural Frequency of Beam Calculator — Complete User Guide & Formula Reference

Step-by-step instructions • All calculation formulas explained • Common mistakes • FAQ • Worked examples

Euler-Bernoulli Theory Timoshenko Theory Multi-Mode Analysis SI & Imperial Units Resonance Checker Structural Engineering

What Is a Natural Frequency of Beam Calculator?

Understanding beam vibration is fundamental to safe structural and mechanical engineering design.

The Natural Frequency of Beam Calculator is an engineering tool that computes the resonant (natural) frequencies at which a structural beam will oscillate when disturbed by an external force, such as wind, machinery vibration, foot traffic, or seismic ground motion. These are the frequencies at which the beam wants to vibrate when left to itself — no sustained energy input required.

If an external force repeatedly applies energy at or near one of these natural frequencies, resonance occurs. Resonance causes vibration amplitudes to grow rapidly, potentially leading to fatigue cracking, excessive deflection, noise, occupant discomfort, or catastrophic structural failure — as famously illustrated by the Tacoma Narrows Bridge collapse (1940).

This calculator uses Euler-Bernoulli and Timoshenko classical beam theory to compute up to 10 vibration modes instantly, eliminating hours of manual calculation.

Typical use cases: Steel floor beams, crane runway girders, footbridges, machine frames, cantilever shelves, turbine blades, vehicle chassis members, and HVAC duct supports.

Key User Pain Points & How This Calculator Solves Them

Real engineers and students face these frustrations daily — here's how the calculator addresses each one.

Complex Manual Calculations Prone to Error

The Euler-Bernoulli frequency formula involves square roots, fourth-power geometry terms, and mode-dependent eigenvalues. A single unit mistake invalidates the entire result.

✓ Auto-computes all terms from raw dimensions

Different Formulas for Each Boundary Condition

Cantilever, simply supported, and fixed-fixed beams all use different βnL eigenvalues. Looking these up from Roark's or textbook tables is slow and error-prone.

✓ 5 boundary conditions with built-in eigenvalue tables

Unit Inconsistency Causing Order-of-Magnitude Errors

Mixing GPa with mm⁴, or kg/m³ with inches, is an extremely common source of catastrophic errors — even for experienced engineers.

✓ One-click SI ↔ Imperial toggle with full auto-conversion

Only Fundamental Mode Computed

Most online calculators only compute f₁. Resonance can occur at higher harmonics (f₂, f₃…), which rotating machinery, pedestrians, or wind can easily excite.

✓ Up to 10 modes calculated simultaneously

No Moment of Inertia Calculator for Standard Sections

Computing I for an I-beam or hollow pipe by hand requires additional sub-calculations, adding setup time and extra steps before reaching the frequency answer.

✓ 5 cross-section types with auto I & A calculation

No Resonance Risk Warning Against Operating Speeds

Engineers often design a beam without checking whether its natural frequency overlaps with the RPM of nearby motors, pumps, or HVAC fans — until vibration becomes a problem.

✓ Built-in resonance checker with Safe / Caution / Danger flags

No Support for Timoshenko Theory (Thick Beams)

Short, stocky beams (L/h < 10) violate the slender beam assumption. Euler-Bernoulli over-predicts frequency for these cases. Timoshenko theory corrects for shear deformation and rotary inertia.

✓ Full Timoshenko correction with shear modulus G and κ

No Damping or Added-Mass Analysis

Real structures have damping (reduces effective frequency) and often carry equipment, people, or pipes. Ignoring these gives overly optimistic (unsafe) frequency predictions.

✓ Damping ratio ζ and point mass inputs with Dunkerley correction

Visual Overview — Boundary Conditions, Mode Shapes & Beam Terminology

Understanding the physical setup before entering numbers prevents the most common input errors.

SIMPLY SUPPORTED (Pinned-Pinned, SS) β₁L = π = 3.1416  |  f₁ lowest of all BCs CANTILEVER (Fixed-Free, CF) β₁L = 1.8751  |  Max deflection at free tip FIXED-FIXED (Clamped-Clamped, CC) β₁L = 4.7300  |  Highest f₁ among common BCs FIXED-PINNED (CP) β₁L = 3.9266  |  Asymmetric mode shape FREE-FREE (FF) β₁L = 4.7300  |  Rigid-body modes at f=0 excluded KEY BEAM PARAMETERS (Rectangular Section Example) L — Beam Length h b Area: A = b × h Inertia: I = b·h³ / 12 Mass/length: μ = ρ × A Rad. of gyration: r = √(I/A) FREQUENCY SUMMARY — Mode 1 vs Mode 2 (Simply Supported) Mode 1 — f₁ = (π)² / (2πL²) √(EI/μ) 1 half-wave | Lowest frequency Mode 2 — f₂ = 4 × f₁ (for SS) 2 half-waves | Second harmonic

Fig. 1 — Five boundary condition configurations with 1st mode shapes and key beam parameters for a rectangular cross-section.

Step-by-Step User Guide — How to Use the Calculator

Follow these steps in order for a complete and accurate calculation. Each step maps to a specific section of the calculator interface.

1

Choose Your Unit System

Before entering any values, click either SI (Metric) or Imperial at the top of the calculator. This switches all unit labels simultaneously — meters ↔ feet, GPa ↔ ksi, kg/m³ ↔ lb/ft³.

  • SI: Length in m, Modulus in GPa, Density in kg/m³, Force in N, Mass in kg
  • Imperial: Length in ft, Modulus in ksi, Density in lb/ft³, Force in lbf, Mass in lb
Mixing SI and Imperial values without switching the toggle first is the single most common error. Always set the unit system BEFORE entering any numbers.
2

Select the Boundary Condition (Support Configuration)

Use the Support Configuration dropdown. This is the most critical input — it determines the eigenvalue βnL used in the formula. Choose based on how the beam ends are physically supported:

  • Simply Supported (SS): Both ends rest on pins/rollers — free to rotate, no end moment. Common in simple spans and bridge girders.
  • Cantilever (CF): One end rigidly bolted to a wall, other end completely free. Common in shelf brackets, balconies, and crane booms.
  • Fixed-Fixed (CC): Both ends are fully welded or embedded — no rotation permitted. Gives highest natural frequency.
  • Fixed-Pinned (CP): One end fully fixed, one end pinned. Occurs in continuous beam spans.
  • Free-Free (FF): Both ends free — represents floating beams, e.g., a beam in mid-air during transport or a rocket fuselage in flight.
Do not confuse "pinned" with "fixed." A pinned end allows rotation but prevents translation. A fixed end prevents both. Using the wrong BC can change the result by a factor of 2 or more.
3

Select Beam Theory

Use the Beam Theory dropdown:

  • Euler-Bernoulli (default): Accurate for slender beams where L/h > 10. Assumes plane sections remain plane and shear deformation is negligible.
  • Timoshenko: Use when L/h < 10 (deep beams, short spans). Accounts for shear deformation and rotary inertia. Requires Shear Modulus G and Shear Correction Factor κ.

If Timoshenko is selected, two additional fields appear: Shear Modulus G and Shear Correction Factor κ.

For a standard steel floor beam (L/h ≈ 20–40), Euler-Bernoulli is appropriate. Only switch to Timoshenko for stocky beams or when accuracy within 5% is required for short-span analysis.
4

Enter Beam Length (L)

Type the total span length in the Beam Length (L) field. Accepted range: any positive value > 0.

  • SI: Enter in metres (m) — e.g., 3.5 for a 3.5 m span
  • Imperial: Enter in feet (ft) — e.g., 12 for a 12 ft span
  • Internally, all values are converted to SI (metres) before calculation

Note: Natural frequency scales as 1/L² — doubling the beam length reduces f₁ by a factor of 4.

5

Select Cross-Section Type & Enter Dimensions

Use the Cross-Section Type dropdown, then enter the required dimensions:

  • Rectangular: Width b (horizontal) & Height h (vertical — in the bending direction). Make sure h is the dimension in the direction of vibration.
  • Circular Solid: Outer diameter d
  • Hollow Pipe: Outer diameter OD & Inner diameter ID. OD must be > ID.
  • I-Beam: Flange width bf, flange thickness tf, web height hw, web thickness tw
  • Custom: Directly enter cross-sectional area A and second moment of area I if you have pre-computed values from CAD or section tables.
For rectangular beams, h must be the dimension in the direction of bending (vertical for floor beams). Swapping b and h can change I by a factor of (h/b)² — for a 50×100 section that's a 4× error in frequency.
6

Select Material or Enter Custom Properties

Click the Material Preset dropdown to auto-fill Young's Modulus E and Density ρ. Available presets:

  • Structural Steel (E = 200 GPa, ρ = 7850 kg/m³)
  • Aluminum 6061 (E = 69 GPa, ρ = 2700 kg/m³)
  • Concrete (E = 30 GPa, ρ = 2400 kg/m³)
  • Timber/Douglas Fir (E = 12 GPa, ρ = 600 kg/m³)
  • Titanium Ti-6Al-4V, Carbon Fiber CFRP, Copper

For non-standard materials, select Custom and manually type E and ρ values.

Young's Modulus must be entered in GPa (SI) or ksi (Imperial) — NOT Pa or psi. Entering 200 Pa instead of 200 GPa produces a frequency 316,000× too low. The unit label next to the field shows the expected unit.
7

(Optional) Open Advanced Options — Damping, Added Mass, Axial Load, Resonance Check

Click the Advanced Options toggle to expand additional inputs:

  • Point Mass (kg or lb): A concentrated mass added at midspan (equipment, motor, person). Uses Dunkerley's approximation to lower the effective frequency.
  • Damping Ratio ζ (0–0.999): Fraction of critical damping. Typical values: steel = 0.01–0.02, concrete = 0.04–0.07, timber = 0.05–0.10. Used to compute the damped natural frequency fd.
  • Axial Load P (N or lbf): Positive = tension (increases frequency), Negative = compression (decreases frequency, approaches buckling). Enter 0 if no axial load.
  • Operating Frequency (Hz): The excitation frequency from machinery or pedestrians. The calculator flags any natural frequency within ±15% as a resonance risk.
8

Click "Calculate Natural Frequency"

The calculator instantly computes all results and switches you to the Results tab, showing:

  • Fundamental frequency f₁ (Hz), angular frequency ω₁ (rad/s), period T (s), damped frequency fd (Hz)
  • Auto-computed section properties: A, I, μ, r, slenderness ratio, flexural rigidity EI
  • Full multi-mode frequency table for modes 1 through N
  • Resonance risk assessment for each mode (if an operating frequency was entered)
9

Export, Copy, or Print Your Results

Use the buttons at the bottom of the Results tab:

  • Copy Results — Copies a plain-text summary of all inputs and results to your clipboard for pasting into reports or emails.
  • Print / Export PDF — Opens the browser print dialog. Use "Save as PDF" in the destination to create a portable PDF report.

All Calculation Formulas — Detailed Derivation & Explanation

Every formula used by the calculator is documented below with variable definitions, units, and physical interpretation.

Formula 1 — Euler-Bernoulli Natural Frequency (Core Formula)

This is the fundamental formula for the n-th mode natural frequency of a uniform prismatic beam, derived from the Euler-Bernoulli beam differential equation of motion:

Euler-Bernoulli Natural Frequency — n-th Mode
\[ f_n = \frac{(\beta_n L)^2}{2\pi L^2} \sqrt{\frac{EI}{\rho A}} \quad \Longleftrightarrow \quad \omega_n = \frac{(\beta_n L)^2}{L^2} \sqrt{\frac{EI}{\rho A}} \]

fn in Hz; ωn in rad/s; relationship: ωn = 2π fn

SymbolQuantitySI UnitImperial UnitPhysical Role
fnNatural frequency of mode nHz (= 1/s)HzOscillations per second; primary output
ωnAngular frequency of mode nrad/srad/sω = 2π f; used in vibration dynamics equations
βnLEigenvalue / frequency constant for mode ndimensionlessdimensionlessRoot of characteristic equation; depends on BC & mode number. See Table in Section 7.
LBeam length (span)mft → converted to mFrequency ∝ 1/L² — most sensitive parameter
EYoung's Modulus (elastic modulus)Pa (entered as GPa)psi (entered as ksi)Material stiffness; frequency ∝ √E
ISecond moment of area (about bending axis)m⁴ft⁴ → converted to m⁴Geometric stiffness; frequency ∝ √I
ρMaterial mass densitykg/m³lb/ft³ → converted to kg/m³Inertia term; frequency ∝ 1/√ρ
ACross-sectional areaft² → converted to m²Combined with ρ → mass per unit length μ = ρA
Sensitivity insight: Frequency scales as f ∝ L⁻² · E^(0.5) · I^(0.5) · ρ⁻⁰·⁵. Cutting the beam length in half quadruples the natural frequency. Doubling E or I only increases it by 41%. Length is by far the most powerful design lever.

Formula 2 — Cross-Section Properties (Automatically Computed)

Rectangular Section (width b, height h in bending direction)
\[ A = b \cdot h \qquad I = \frac{b \, h^3}{12} \qquad r = \sqrt{\frac{I}{A}} = \frac{h}{2\sqrt{3}} \]

h is the dimension parallel to the bending axis. For a beam bending vertically, h is the vertical depth.

Circular Solid Section (diameter d)
\[ A = \frac{\pi d^2}{4} \qquad I = \frac{\pi d^4}{64} \]
Hollow Circular Pipe (outer diameter OD, inner diameter ID)
\[ A = \frac{\pi (OD^2 - ID^2)}{4} \qquad I = \frac{\pi (OD^4 - ID^4)}{64} \]

OD must be strictly greater than ID. If ID ≥ OD, the calculator will report a geometry error.

I-Beam / Wide Flange (flange width bf, flange thickness tf, web height hw, web thickness tw)
\[ h_{total} = h_w + 2 t_f \] \[ A = 2 b_f t_f + h_w t_w \] \[ I = \frac{b_f \, h_{total}^3 - (b_f - t_w) \, h_w^3}{12} \]

This is the standard parallel-axis / subtraction method for doubly-symmetric I-sections about the major (strong) axis.

Formula 3 — Damped Natural Frequency

When a structure has internal material damping (or added dampers), the effective frequency at which it actually oscillates is slightly lower than the undamped natural frequency:

Damped Natural Frequency
\[ f_d = f_n \sqrt{1 - \zeta^2} \]

For ζ = 0.05 (5% damping, typical concrete): fd = 0.9987·fn — only 0.13% lower. For ζ = 0.2 (20%): fd = 0.98·fn. Damping has a minor effect on frequency but a major effect on vibration amplitude at resonance.

SymbolQuantityTypical RangeNotes
fdDamped natural frequencyHzAlways ≤ fn
ζDamping ratio0 to <1ζ = c / ccr; ζ = 1 is critically damped (no oscillation)
fnUndamped natural frequencyHzFrom Euler-Bernoulli / Timoshenko formula above

Formula 4 — Timoshenko Beam Correction for Short/Thick Beams

The Euler-Bernoulli theory over-estimates frequency for short beams because it ignores shear deformation and rotary inertia. The Timoshenko correction factor reduces the EB frequency:

Timoshenko Frequency Correction
\[ \omega_{Tim} = \omega_{EB} \cdot \underbrace{\frac{1}{\sqrt{1 + (\beta_n r)^2 \left(\dfrac{E}{\kappa G} + 1\right)}}}_{\text{correction factor} \leq 1} \]

where r = √(I/A) is the radius of gyration, κ is the shear correction factor, and G is the shear modulus. The correction factor is always ≤ 1, meaning Timoshenko frequency ≤ Euler-Bernoulli frequency.

SymbolQuantitySI UnitTypical Values
GShear modulusPa (entered as GPa)Steel: 77 GPa | Alum: 26 GPa | Concrete: ~12 GPa
κShear correction factordimensionlessRect: 5/6 ≈ 0.833 | Circular: 0.9 | I-beam: ~0.44
rRadius of gyration = √(I/A)mIndicates how mass is distributed about bending axis

Formula 5 — Axial Load Effect on Natural Frequency

An axial tensile force stiffens a beam (increases frequency), while a compressive force softens it (decreases frequency, approaching zero at the buckling load):

Frequency Modified by Axial Load
\[ f_{n,P} = f_n \sqrt{1 + \frac{P}{P_{cr,n}}} \qquad \text{where} \qquad P_{cr,n} = \frac{(\beta_n L)^2 \, EI}{L^2} \]

P > 0 = tension (increases f); P < 0 = compression (decreases f). When P = −Pcr,1, frequency → 0 (buckling onset). Critical buckling load Pcr,1 for Simply Supported = π²EI/L² (Euler buckling).

Formula 6 — Dunkerley's Method for Added Point Mass

When a concentrated mass is added to the beam (e.g., a motor or equipment), the effective natural frequency drops. Dunkerley's approximation combines the beam's own frequency with the frequency as if the beam were massless but carried the point load:

Dunkerley's Approximation — Point Mass at Midspan
\[ \frac{1}{f_{eff}^2} \approx \frac{1}{f_n^2} + \frac{1}{f_m^2} \quad \text{where} \quad f_m^2 = f_n^2 \cdot \frac{\mu L}{\mu L + m_{point}} \]

μL = total beam mass (kg); mpoint = added point mass (kg). This is applied to the fundamental mode only. For higher modes with added mass, full eigenvalue analysis (FEA) is recommended.

Formula 7 — Period of Vibration

Period T
\[ T_n = \frac{1}{f_n} \quad \text{(seconds)} \]

Period T is the time for one complete oscillation cycle. Used in earthquake engineering (response spectra) and fatigue life estimation (cycles per second).

Input Units & Accepted Values — Validation Reference

Use this table to verify your inputs are in the correct units before calculating. All values must be positive and non-zero unless noted.

Parameter SI Input Unit Imperial Input Unit Valid Range Common Error
Beam Length L metres (m) feet (ft) > 0 Entering mm instead of m (×1000 error)
Section dimensions (b, h, d, etc.) metres (m) feet (ft) > 0; OD > ID for pipes Entering mm instead of m (×1000 error in I)
Young's Modulus E GPa (e.g., 200 for steel) ksi (e.g., 29,000 for steel) > 0 Entering Pa or psi without unit conversion
Density ρ kg/m³ (e.g., 7850 for steel) lb/ft³ (e.g., 490 for steel) > 0 Entering g/cm³ instead of kg/m³
Shear Modulus G GPa (e.g., 77 for steel) ksi (e.g., 11,200 for steel) > 0 (Timoshenko only) Leaving at steel default when using aluminum
Shear Correction Factor κ Dimensionless (no unit) 0.1 – 1.0 Using 0.833 (rectangular) for circular sections
Damping Ratio ζ Dimensionless (decimal, NOT %) 0 to 0.999 Entering 5 instead of 0.05 for 5% damping
Point Mass m kg lb ≥ 0 Entering kN load instead of mass in kg
Axial Load P N lbf any real number; P < 0 = compression Entering kN without converting (×1000 error)
Operating Frequency Hz (always, regardless of unit system) > 0 (optional) Entering RPM instead of Hz (divide RPM by 60)
Custom Area A ft² > 0 Entering mm² instead of m²
Custom Inertia I m⁴ ft⁴ > 0 Entering mm⁴ or cm⁴ instead of m⁴
Converting RPM to Hz: Many motors and pumps are rated in RPM. To enter the correct operating frequency: Hz = RPM ÷ 60. For example, a 1200 RPM motor = 20 Hz. A 3600 RPM motor = 60 Hz.

Eigenvalue (βnL) Reference Table for All Boundary Conditions

The βnL values (also called frequency factors or modal constants) are the most critical input to the natural frequency formula. They are roots of the characteristic equation for each boundary condition.

Boundary Condition Mode 1 Mode 2 Mode 3 Mode 4 Mode 5 Higher Modes (n ≥ 3)
Simply Supported (SS) π = 3.1416 2π = 6.2832 3π = 9.4248 4π = 12.5664 5π = 15.7080
Cantilever (CF) 1.8751 4.6941 7.8548 10.9955 14.1372 (2n−1)π/2 ≈ exact for n ≥ 5
Fixed-Fixed (CC) 4.7300 7.8532 10.9956 14.1372 17.2788 (2n+1)π/2 ≈ exact for n ≥ 3
Fixed-Pinned (CP) 3.9266 7.0686 10.2102 13.3518 16.4934 (4n+1)π/4 ≈ exact for n ≥ 3
Free-Free (FF) 4.7300 7.8532 10.9956 14.1372 17.2788 Same as CC (symmetric)

Note: For Free-Free beams, there are two rigid body modes at f = 0 Hz (pure translation and pure rotation) before the first elastic mode at β₁L = 4.7300. The calculator excludes these rigid-body modes.

Frequency Ratios Relative to Mode 1

Boundary Conditionf₂/f₁f₃/f₁f₄/f₁f₅/f₁
Simply Supported (SS)4.09.016.025.0
Cantilever (CF)6.2717.5534.3956.84
Fixed-Fixed (CC)2.765.408.9313.34
Fixed-Pinned (CP)3.246.7611.5317.64
Free-Free (FF)2.765.408.9313.34

Example: For a simply supported beam with f₁ = 5 Hz, the second mode f₂ = 20 Hz and third mode f₃ = 45 Hz. A machine running at 18–22 Hz would be near resonance with Mode 2.

Material Property Reference Table

Pre-loaded values used by the material presets. Use these as defaults for custom materials when manufacturer data is unavailable.

Material E (GPa) ρ (kg/m³) G (GPa) ν (Poisson) Typical ζ Notes
Structural Steel 200 7850 77 0.30 0.01–0.02 E430, S275, A36, S355
Aluminum 6061-T6 69 2700 26 0.33 0.01–0.02 High strength-to-weight ratio
Concrete (Normal) 25–35 2400 12 0.20 0.04–0.07 E depends on f'c; use 30 GPa for C30
Timber / Douglas Fir 12 600 0.75 0.37 0.05–0.10 Parallel-to-grain; highly variable
Titanium Ti-6Al-4V 116 4430 44 0.34 0.01 Aerospace alloy; high E/ρ ratio
Carbon Fiber CFRP (UD) 135 1600 7 0.30 0.005–0.01 Unidirectional laminate, fiber direction
Copper 110 8940 41 0.34 0.02 High density limits frequency
Steel (Imperial) 29,000 ksi 490 lb/ft³ 11,200 ksi 0.30 0.01–0.02 ASTM A36 / A992

⚙ Accuracy Note & Theory Limitations — Read Before Relying on Results

  • Euler-Bernoulli accuracy: Results are within ~1–2% of exact solutions for beams with slenderness ratio L/h > 10. For L/h < 10, switch to Timoshenko theory. For L/h < 5, use FEA.
  • Uniform beam assumption: This calculator assumes a prismatic (constant cross-section) beam along its full length. Tapered, stepped, or composite beams require numerical FEA methods for accurate results.
  • Boundary condition idealization: Real support conditions are never perfectly rigid or perfectly pinned. Partial fixity, foundation flexibility, and joint stiffness can shift actual frequencies by 5–25% from theoretical values.
  • Dunkerley for added mass: The point-mass correction using Dunkerley's method is an approximation (conservative — it under-estimates frequency). For multiple added masses or off-center masses, results may differ from FEA by up to 10–15%.
  • Axial load formula validity: The axial load correction is valid for P < 0.5·Pcr. Approaching the buckling load, the formula becomes less accurate and FEA or specialized stability analysis should be used.
  • Not a substitute for FEA or code compliance: This tool is for preliminary design, education, and quick checks. Critical structural designs should be verified by a licensed engineer using full FEA and applicable codes (AISC, Eurocode, ASCE, etc.).
 

Frequently Asked Questions (FAQ)

Answers to the most common questions from engineers, students, and designers using this calculator.

They are the same thing in the context of beams and structures. The natural frequency is the frequency at which the beam oscillates freely when disturbed. Resonance occurs when an external forcing frequency matches one of the natural frequencies, causing energy to build up and amplitudes to grow. "Resonance frequency" just means the natural frequency that is being excited by an external source.
The most common causes are: (1) Unit mismatch — verify all inputs use the unit shown next to each field. (2) Wrong boundary condition — partial fixity in real structures means actual frequencies fall between fully-pinned and fully-fixed theoretical values. (3) Short beam not using Timoshenko theory — for L/h < 10, switch to Timoshenko. (4) Non-uniform cross-section — this calculator assumes constant section properties along the full length.
Divide the RPM value by 60: Hz = RPM ÷ 60. Examples: 1800 RPM = 30 Hz; 3000 RPM = 50 Hz; 3600 RPM = 60 Hz. For multi-blade machinery (fans, compressors), also check blade-pass frequencies: fblade = (RPM × number of blades) ÷ 60.
CAUTION means the natural frequency of that mode is within 5–15% of your entered operating frequency. This is the engineering warning zone — vibration amplitudes will be elevated but not necessarily catastrophic. Industry practice typically requires a 20% frequency separation (fn / foperating > 1.2 or < 0.8) between any natural frequency and operating speed. DANGER means the separation is less than 5% — redesign is strongly recommended.
Since f ∝ 1/L², the most effective strategy is to reduce the span length (add intermediate supports). Other options: (1) Increase cross-section depth h (I scales as h³, so f ∝ h^1.5). (2) Change boundary conditions from pinned to fixed ends (β₁L for CC = 4.73 vs π = 3.14 for SS — that's 2.27× higher frequency). (3) Add pre-tension via cables or bolts (increases frequency via axial load effect). (4) Remove mass (reduce self-weight or added loads).
Typical damping ratios ζ by material and structural system: Structural steel (welded): 0.01–0.02. Steel (bolted): 0.02–0.04. Reinforced concrete: 0.04–0.07. Pre-stressed concrete: 0.02–0.05. Timber: 0.05–0.10. Composite steel-concrete: 0.02–0.04. Soil/foundations: 0.05–0.20. For most preliminary calculations, damping has a minor effect on frequency (less than 1% for ζ < 0.1) but significantly affects vibration amplitude at resonance.
Yes. Select the appropriate material preset (Concrete or Timber) or enter custom E and ρ values. For concrete, keep in mind that cracked concrete has a lower effective E (typically 0.4–0.7× the uncracked value). For timber, E parallel to grain can vary by ±20% due to natural variability — consider using the lower bound for conservative design. For reinforced concrete, the composite E and ρ should be used (transformed section approach), which may require custom entry.
The slenderness ratio L/r (where r = √(I/A) is the radius of gyration) indicates how "slender" the beam is relative to its cross-section. L/r > 100: Very slender — Euler-Bernoulli theory is fully valid; buckling and lateral-torsional buckling may be concerns. L/r = 30–100: Moderately slender — Euler-Bernoulli appropriate. L/r < 30: Short/stocky — switch to Timoshenko theory for more accurate frequency results. L/r < 10: Deep beam — the simple beam theory may not apply; use FEA.
Click the Print / Export PDF button on the Results tab. In the print dialog, choose Save as PDF as the destination (available in Chrome, Edge, Firefox, and Safari). For the best layout, use landscape orientation and ensure "Background graphics" is enabled in print settings to preserve the colour coding of results. The PDF will include all input parameters, section properties, and the full multi-mode frequency table.
It comes down to the β₁L eigenvalue. For a cantilever, β₁L = 1.8751. For a simply supported beam, β₁L = π = 3.1416. Since frequency ∝ (β₁L)², the simply supported beam has a fundamental frequency (3.1416/1.8751)² = 2.81× higher than a cantilever of the same length, material, and cross-section. Physically, the fixed end provides more restraint and effectively "shortens" the equivalent span for vibration purposes — but the free end of a cantilever has maximum displacement and minimum constraint, giving a lower effective stiffness.

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