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.
Calculated output
Results
- Sum of isolated static deflections
- Estimated critical angular speed
- Estimated first lateral natural frequency
- Lowest active partial critical speed
- Reduction from lowest partial speed
- Active isolated case count
- Operating-to-critical speed ratio
- Operating-speed position relative to estimate
- Absolute separation from estimate
- User review-band lower speed
- User review-band upper speed
Valid Dunkerley first critical-speed estimate
- 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:
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% |
- Sum the isolated deflections:
Σδᵢ = 0.25 + 0.60 + 0.15 = 1.00 mm. - Calculate the combined angular frequency:
ωD = √(9,806.65 / 1.00) = 99.028531 rad/s. - Convert to frequency:
fD = 15.760880 Hz. - Convert to critical speed:
nD = 945.652815 rpm. - The combined estimate is
22.5403%below the lowest active partial speed of1,220.832535 rpm. - At
600 rpm, the speed ratio is0.634482and the operating point is36.5518% belowthe estimate. - 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.
- Karlsruhe Institute of Technology — Dynamics of Rotating Machines — University text deriving Dunkerley's equation from influence coefficients, isolated mass cases, and reciprocal partial natural frequencies.
- Union College MER419 — Critical Frequency lecture — University machine-design material showing that each Dunkerley shaft deflection is calculated from one mass acting individually and combining the resulting partial frequencies.
- NIST Guide to the SI — conversion factors and standard gravity — Official reference listing standard acceleration of free fall as 9.80665 m/s² and supporting the length conversions used by the calculator.
- NASA Technical Reports Server — Critical Speed Analysis — Government analysis illustrating why rotating-assembly critical-speed predictions depend on the complete shaft, bearing, and support model.