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Ideal one-dimensional linear model

Equivalent Linear Spring Stiffness

Combine two to five positive tangent spring rates in a true one-dimensional series or parallel arrangement. Optional natural frequency uses an ideal undamped single-degree-of-freedom model.

SeriesParaleloStrict SI inputOptional SDOF

Limite do modelo: all active elements must be linear about the operating point and act along the same generalized coordinate. Series requires the same force through every element; parallel requires the same deflection. Preload, geometric leverage, bending, contact changes, damping and spring/mount mass are not included.

Equivalent ideal model

Equivalent stiffness keq
SI stiffness
Imperial conversion
Compliance 1/keq
Natural frequency fn
Angular frequency ωn

Parallel: keq = Σki   (common deflection, forces add)
Series: 1/keq = Σ(1/ki)   (common force, deflections add)

MIT OpenCourseWare Precision Engineering Principles states these compliance/stiffness addition rules. A separate MIT solid-mechanics laboratory note derives the two-spring series result from equilibrium and compatibility.

ωn = √(keq/m),   fn = ωn/(2π)

The frequency result applies only to a rigid effective mass on massless linear springs with one degree of freedom and no damping. MIT Mechanics and Materials states this boundary explicitly. For real isolators, include the effective mass of mounts/springs, geometry, damping and all coupled modes.

Unit correction: input is always N/mm and kg. Results also show N/m and lbf/in, using exact SI definitions: 1 lbf=4.4482216152605 N and 1 in=25.4 mm. The old toggle reinterpreted unchanged numbers and could alter physical stiffness by 5.71×.

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Reference idealization only; validate the actual force–deflection curve and effective dynamic mass. Scientific review: July 2026.

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