Shafts · Rotordynamic screening

Mechanical Engineering Calculators: Dunkerley Multi-Mass Shaft Critical Speed Calculator

Mechanical Engineering Calculators for estimating first shaft critical speed from up to four isolated single-mass gravity deflections using Dunkerley's equation.

Reference calculator #027

Enter isolated single-mass gravity deflections

Inputs stay in your browser. Values are normalized to canonical units before calculation.

Deflection at this rotor station when only this case weight acts; do not enter the total deflection from all rotor weights.

Deflection at this rotor station when only this case weight acts; do not enter the total deflection from all rotor weights.

Deflection at this rotor station when only this case weight acts; do not enter the total deflection from all rotor weights.

Deflection at this rotor station when only this case weight acts; do not enter the total deflection from all rotor weights.

Enter the steady or evaluated shaft speed in rpm; zero is valid for a stationary comparison.

User-selected screening band from 0% through 100%; it is not a universal acceptance margin.

Calculated output

Results

dunkerley-critical-speed/1.0.0
Dunkerley first critical-speed estimate945.652815 rpm
Sum of isolated static deflections
1 mm
Estimated critical angular speed
99.028531 rad/s
Estimated first lateral natural frequency
15.76088 Hz
Lowest active partial critical speed
1220.832535 rpm
Reduction from lowest partial speed
22.5403%
Active isolated case count
3
Operating-to-critical speed ratio
0.634482×
Operating-speed position relative to estimate
36.5518% below
Absolute separation from estimate
36.5518%
User review-band lower speed
756.522252 rpm
User review-band upper speed
1134.783378 rpm

Valid Dunkerley first critical-speed estimate

Dunkerley isolated-case contributions and operating-speed comparisonFour bars show each isolated single-mass deflection's share of the Dunkerley deflection sum. A separate speed axis compares operating speed with the estimated first critical speed and the user-selected review band.Isolated-case shares of ΣδᵢΣδᵢ = 1 mmLowest partial speed = 1220.832535 rpm25%Case 1δ = 0.25 mmnᵢ = 1891.305631 rpm60%Case 2δ = 0.6 mmnᵢ = 1220.832535 rpm15%Case 3δ = 0.15 mmnᵢ = 2441.66507 rpm0%Case 4δ = 0 mmnᵢ = DisabledOperating-speed comparisonReview band: ±20%0 rpmEstimated nD = 945.652815 rpmOperating n = 600 rpmReview range: 756.522252 rpm to 1134.783378 rpmSpeed ratio = 0.634482×Operating point: 36.5518% below
Bars show isolated-deflection terms in the reciprocal-frequency sum. They are not shaft positions, combined static deflections, or vibration amplitudes.
Scope and assumptions
  • Each entered δᵢ is the static deflection at the applicable rotor station caused by that rotor weight acting alone; inertial effects of every other rotor mass are omitted from that partial case.
  • All isolated cases use the same linear-elastic shaft, bearing-support model, boundary conditions, lateral direction, and unit basis, so their reciprocal-frequency terms can be combined.
  • Dunkerley’s method estimates the first lateral critical speed from partial single-mass cases and is generally conservative for the ideal linear model; it is not an exact modal solution.
  • Distributed shaft mass is excluded unless its effect is evaluated separately by an applicable method; do not enter a total multi-weight deflection or an arbitrary operating-load deflection.
  • Bearing, seal, support, and foundation flexibility are included only to the extent that each isolated static-deflection case represents them consistently.
  • Damping, gyroscopic effects, speed-dependent coefficients, cross-coupling, higher modes, unbalance response, vibration amplitude, and transient run-up or coast-down are excluded.
  • The user-selected review band is a screening aid, not a universal separation-margin requirement or an acceptance criterion.

Calculation engine: dunkerley-critical-speed/1.0.0

Dunkerley multi-mass critical-speed equation

Dunkerley’s method combines partial natural frequencies obtained by considering each lumped rotor mass separately. For case i, determine the gravity static deflection at that mass location with only that mass weight acting. The partial frequency and combined estimate are:

1 / ωD² ≈ Σ(1 / ωᵢ²)
ωᵢ = √(g / δᵢ)
ωD ≈ √(g / Σδᵢ)
nD = 60ωD / (2π)
Symbol Meaning Calculator basis
δᵢ Static deflection from isolated single-mass case i mm internally
ωᵢ Partial angular frequency with only mass i present rad/s
ωD Combined Dunkerley first-frequency estimate rad/s
nD Estimated first synchronous critical speed rpm
g Standard acceleration due to gravity 9,806.65 mm/s²

The published relationship is often described as an underestimate of the fundamental frequency for the ideal linear multi-degree-of-freedom model. That mathematical tendency does not turn the output into a guaranteed safe lower bound for a real machine with uncertain bearings, supports, damping, geometry, and operating conditions.

The isolated-case requirement

Each field represents a separate structural load case. For δ₁, apply only rotor weight 1 and measure or calculate deflection at its own station. Repeat independently for every other rotor weight. Preserve the same shaft geometry, elastic properties, bearing and support boundary conditions, and lateral direction.

Do not enter:

  • total deflection with all rotor weights acting together;
  • deflection from transmitted gear force, belt pull, chain tension, process force, or torque;
  • maximum shaft deflection at a coordinate different from the mass station;
  • a mixture of deflections obtained from different support models;
  • arbitrary values selected to reach a target speed.

Calculator #026 uses the total multi-weight deflection field required by Rayleigh’s energy method. Those yᵢ inputs are deliberately not transferred to #027 because their physical definitions are different.

Worked example

Use three active isolated cases and one disabled case:

Case Isolated gravity deflection Partial critical speed Share of Σδᵢ
1 0.25 mm 1,891.305631 rpm 25%
2 0.60 mm 1,220.832535 rpm 60%
3 0.15 mm 2,441.665070 rpm 15%
4 0 mm Disabled 0%
  1. Sum the isolated deflections: Σδᵢ = 0.25 + 0.60 + 0.15 = 1.00 mm.
  2. Calculate the combined angular frequency: ωD = √(9,806.65 / 1.00) = 99.028531 rad/s.
  3. Convert to frequency: fD = 15.760880 Hz.
  4. Convert to critical speed: nD = 945.652815 rpm.
  5. The combined estimate is 22.5403% below the lowest active partial speed of 1,220.832535 rpm.
  6. At 600 rpm, the speed ratio is 0.634482 and the operating point is 36.5518% below the estimate.
  7. The default ±20% review range is 756.522252 to 1,134.783378 rpm, so 600 rpm lies outside it.

The contribution bars visualize δᵢ / Σδᵢ. A larger bar identifies a larger reciprocal-frequency contribution and therefore a stronger reduction of the combined estimate. It does not represent physical rotor position or vibration amplitude.

Cross-check with the single-deflection relationship

Because substituting ωᵢ = √(g/δᵢ) reduces the reciprocal-frequency sum to ωD = √(g/Σδᵢ), Calculator #025 can reproduce the #027 numerical result using the summed isolated deflection. The related-action link transfers this sum together with operating RPM and the review band.

That cross-check confirms the algebra and unit conversion only. It does not validate whether the individual deflections were generated correctly or whether Dunkerley’s assumptions fit the rotor-bearing-support system.

Engineering scope and limitations

This calculator provides four input slots and combines up to four positive isolated gravity-deflection cases. It excludes:

  • derivation or verification of the isolated deflections and influence coefficients;
  • direct input of weights, masses, stiffnesses, shaft geometry, or partial frequencies;
  • distributed shaft mass and a separate bare-shaft critical-speed term;
  • overhung, stepped, branched, coupled, anisotropic, cracked, or nonlinear rotor behavior unless independently represented by a valid method;
  • higher bending modes, gyroscopic splitting, speed-dependent bearing or seal coefficients, cross-coupling, fluid-induced instability, rubs, and nonlinear clearances;
  • unbalance-response amplitude, resonance stress, orbit, phase, amplification, damping ratio, run-up or coast-down response, and protection settings;
  • universal separation criteria, permissible operating ranges, pass/fail classification, standards compliance, or engineering approval.

Use an applicable transfer-matrix, finite-element, modal, or full rotordynamic analysis when the machine cannot be represented by consistent isolated single-mass cases. Confirm predicted critical speeds against qualified engineering review and suitable test or operational evidence before releasing a design or operating through a critical-speed region.

Frequently asked questions

What deflection does each Dunkerley input require?

Each δᵢ must be the static deflection at the applicable rotor station when only that rotor weight acts. The other rotor masses must be absent from that partial load case.

Can I copy the total station deflections from the Rayleigh calculator?

No. Calculator #026 requires the total deflection at every station with all rotating weights acting together. Dunkerley's equation requires separate self-deflection cases with one rotor weight acting at a time.

Why are rotating weights not separate calculator inputs?

The isolated deflection already contains the effect of its associated weight and local flexibility. Once each verified δᵢ is known, the partial frequency is √(g/δᵢ), so entering weight again would be redundant and could imply that the calculator derives deflection.

What happens when only one case is active?

The equation reduces to ω = √(g/δ), which is the single-static-deflection relationship used by Calculator #025. A warning makes this reduction explicit.

Does Dunkerley's estimate include shaft self-weight?

Not in this implementation. The four fields represent isolated lumped rotor-weight cases. Distributed shaft mass requires a separately justified shaft-only term or a more suitable transfer-matrix, finite-element, or rotordynamic model.

Is the Dunkerley estimate a safe operating limit?

No. It is a first-mode screening estimate. The user-selected review band is not a standard or pass/fail criterion, and the calculator does not predict vibration amplitude, resonance stress, damping, or safe passage through a critical speed.

References and review status

Reviewed . References support Dunkerley's reciprocal-frequency relationship, the isolated single-mass deflection requirement, and standard gravity. They do not establish the input deflections, actual machine critical speeds, vibration response, a universal separation margin, or operating approval.