How much of the base’s harmonic motion reaches the equipment — displacement transmissibility for a spring-mass-damper system under base excitation.
/ INPUT
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{{ zetaStr }}
0.01 · light0.40 · heavy
NAT. FREQ fₙ
{{ fnStr }}
Hz
FREQ RATIO r
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f / fₙ
TRANSMISSIBILITY T
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X / Y · dimensionless
ISOLATION
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efficiency
TRANSMITTED
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of base amplitude
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TRANSMISSIBILITY vs FREQUENCY RATIOCH1 ▸ T(r)OP {{ opChip }}
/ HOW IT WORKSTHEORY · BASE EXCITATION
When equipment is mounted on a vibrating surface (floor, vehicle, building), the support undergoes harmonic base motion y(t) = Y sin(ωt). The mount — spring stiffness k and viscous damper coefficient c in parallel — controls how much motion reaches the equipment. The displacement transmissibility T = X/Y (equipment amplitude over base amplitude) is:
TDisplacement transmissibility — ratio of equipment amplitude X to base amplitude Y (T < 1: equipment moves less than the base)rFrequency ratio — base excitation frequency divided by natural frequency, f / fn (isolation requires r > √2 ≈ 1.41)ζDamping ratio — c / (2√km), fraction of critical damping (dimensionless; typical mount range 0.05–0.15)fBase excitation frequency — frequency of the harmonic floor or support motion (Hz)fnUndamped natural frequency of the mount–equipment system, ωn / 2π (Hz)kTotal mount stiffness — combined spring constant of all isolators (N/mm)mEquipment mass supported by the mounts (kg)δStatic deflection of mounts under supported weight, δ = mg/k (mm); equivalent way to specify stiffness
Below r = √2 the mounts amplify base motion, with resonance (r = 1) as the worst case. True isolation begins above r = √2 — the design target r ≥ 3 limits equipment amplitude to less than 13 % of the base amplitude for light damping.
BASE EXCITATION MODEL
⊕ ENGINEER’S NOTE
More damping tames the resonance peak during start-up but slightly raises T at high r — it reduces isolation in the operating band.
Choose ζ to safely survive resonance on the way up to operating speed, not to maximise steady-state isolation.