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Reference worksheet · documented equivalent stiffness · linear SDOF

Documented Elastomer-Mount Linear-Stiffness Worksheet

Calculate linear-model gravity deflection and undamped natural frequency from a documented or measured equivalent axial stiffness and the supported mass assigned to the same coordinate.

no Shore-only stiffnessexact SI/U.S. unitsexplicit stiffness conditionno isolation verdict
Shore A hardness is not a mount spring constant. ISO 48-4 defines an indentation-hardness test. ASTM D2240 describes durometer hardness as an empirical control test and states that no simple relationship exists to a fundamental material property. Geometry, bonding, preload, strain amplitude, frequency, temperature, ageing and compound construction must come from product data or testing.

Controlled inputs

Use an equivalent stiffness for the actual mount assembly, axis, preload and boundary condition. A force/deflection pair yields only a secant stiffness for that pair.

Direct mode: enter the equivalent linear stiffness for the selected translational coordinate.
Mass, not force. Include only the effective mass represented by the one-degree-of-freedom model.
Required model confirmation

Reference linear-model result

Equivalent stiffness K
Linear-model gravity deflection δlin
Undamped natural frequency fn
Supported mass M
Reference weight M g0
No Shore-to-stiffness estimate, load-capacity check, transmissibility, damping, resonance margin, service-life or safe-selection verdict is produced.

Equations and model boundary

For a positive equivalent translational stiffness K and effective supported mass M in a linear single-degree-of-freedom model:

Ksec = F/Δ · δlin = M g0/K · ωn = √(K/M) · fn = ωn/(2π)

The worksheet uses conventional standard gravity g0 = 9.80665 m/s² exactly only for the reference weight and gravity-deflection identity. Local gravity can be substituted outside this worksheet when required.

A force/deflection pair produces a secant stiffness between the two stated points. It is not automatically the tangent stiffness governing small perturbations and it is not automatically the dynamic storage stiffness governing a vibration test.

Exact unit normalization

Calculation is performed in N/m, kg and m. The exact bases are 1 in = 0.0254 m, 1 lbm = 0.45359237 kg and 1 lbf = 0.45359237×9.80665 N. Therefore 1 N/mm = 5.710147154733… lbf/in, not 0.00571015 lbf/in.

Reference check

УлазиКδlinfn
K = 100 N/mm; M = 100 kg100000 N/m9.80665 mm5.03292121045 Hz
F = 1000 N; Δ = 10 mm; M = 100 kg100 N/mm9.80665 mmsame linear model

What Shore A does and does not establish

ISO 48-4:2018, confirmed in 2024, specifies an indentation-hardness measurement method using Shore durometers. It does not publish a universal spring-stiffness equation for a finished mount in its public scope. ASTM D2240-15(2021) explicitly characterizes durometer hardness as an empirical control test and says no simple relationship exists between the measured indentation hardness and a fundamental material property.

A historical Gent correlation between Shore hardness and Young’s modulus is an approximate material correlation, not a complete mount model. Turning it into a mount stiffness additionally requires compound response, geometry, bonding/friction, compressibility and strain assumptions. This worksheet therefore does not implement that correlation.

Static versus dynamic elastomer behavior

ASTM D5992-96(2024) covers vibratory methods for measuring rubber stiffness, damping and dynamic modulus, including tests on full-scale products. A static catalog stiffness cannot silently be treated as dynamic storage stiffness. Record temperature, preload, frequency and amplitude with every stiffness value.

Source classification

ClaimКласификацијаInspected source
Shore A is indentation hardness measured by a durometerCurrent standard scope; no stiffness equation inferredISO 48-4:2018, edition 1, current and confirmed 2024
Durometer hardness is empirical and has no simple relationship to a fundamental propertyCurrent ASTM significance/use statementASTM D2240-15(2021), active; revision work item separately under development
Dynamic rubber stiffness/damping/modulus require vibratory measurement methods and conditionsCurrent ASTM guide scopeASTM D5992-96(2024), active
δ = Mg/K and ωn = √(K/M)General linear SDOF mechanics; not an ISO mount-selection formulaMIT OCW 2.003SC Engineering Dynamics, Recitation 10, rendered page 1
inch, pound-mass and pound-force normalizationMetrology and exact definitionsNIST SP 811 Appendix B.8; BIPM 3rd CGPM Resolution 2

ISO 48-4:2018 official card — edition, status, confirmation and public scope.

ASTM D2240-15(2021) — active durometer-hardness method and public significance/use statement.

ASTM D5992-96(2024) — active dynamic-testing guide and public scope.

MIT OCW Recitation 10 notes — linear spring gravity deflection and undamped natural frequency.

NIST SP 811 Appendix B.8 и BIPM 3rd CGPM Resolution 2 — exact unit and conventional-gravity basis.

Accessed: 15 July 2026. The MIT PDF page was rendered and visually inspected. Only public ISO/ASTM scope/status text was used; no inaccessible clause, coefficient or limit was invented.

Reference model only. Final mount selection requires manufacturer load-deflection/dynamic-stiffness data or a controlled product test, plus checks for allowable load/strain, stability, creep, temperature, environment, fatigue, damping, resonance and failure consequences.
Revision: scientific audit 2026-07-15 · English source page · Linear SDOF reference only · Preserve the source and condition of K with the result.
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