PhysSandbox
Classical MechanicsWaves & SoundElectricity & MagnetismOptics & LightGravity & OrbitsLabs
🌙Astronomy & The Sky🌡️Thermodynamics🌍Biophysics, Fluids & Geoscience📐Math Visualization🔧Engineering🧪Chemistry

Related simulators

Similar topics nearby (including related fields) — or browse all 48 in Engineering.

View category →
NewUniversity / research

Jeffcott Rotor Critical Speed

Launch Simulator

Single disk on a flexible shaft: ω_n = √(k/m), unbalance response, whirl orbit, phase lag, and critical-speed crossing.

NewUniversity / research

Torsional Drivetrain Resonance

Launch Simulator

Two-inertia torsional drivetrain: shaft stiffness and damping, twist angle, first natural mode, resonance response, and optional backlash deadzone.

NewUniversity / research

AM / FM Modulation

Launch Simulator

Carrier + message: AM envelope vs FM phase; waveform and DFT spectrum snapshot.

NewSchool

Bridge Resonance (1-D mode)

Launch Simulator

Damped modal oscillator with harmonic drive: sweep ω near √(k/m) — presets for cadence-like and low-ζ peaks.

NewUniversity / research

Heat Exchanger ε-NTU

Launch Simulator

Parallel and counter-flow heat exchanger calculator: NTU = UA/Cmin, capacity ratio Cr, effectiveness, heat transfer, and outlet temperatures.

NewUniversity / research

Hertzian Contact Stress

Launch Simulator

Sphere or cylinder on a flat: effective modulus, contact patch, peak pressure p0, elastic approach, and subsurface shear estimate.

PhysSandbox

Interactive physics, chemistry, and engineering simulators for students, teachers, and curious minds.

Physics

  • Classical Mechanics
  • Waves & Sound
  • Electricity & Magnetism

Science

  • Optics & Light
  • Gravity & Orbits
  • Astronomy & The Sky

More

  • Thermodynamics
  • Biophysics, Fluids & Geoscience
  • Math Visualization
  • Engineering
  • Chemistry

© 2026 PhysSandbox. Free interactive science simulators.

PrivacyTermsContact
Home/Engineering/Vibration Isolation Transmissibility

Vibration Isolation Transmissibility

SDOF base-excitation isolator: transmissibility T(r,ζ), resonance peak, phase lag, and the isolation region above r = √2.

Isolator parameters

0.12
2.6
4 Hz
8 mm

For base displacement excitation, isolation begins when T < 1, which occurs above r = sqrt(2). Damping suppresses the resonance peak but raises high-frequency transmission.

Measured values

Transmissibility T0.20
Mass amplitude X1.6 mm
Phase lag142 deg
Forcing frequency10.4 Hz

This is the standard linear SDOF isolator. Real mounts add nonlinear stiffness, stroke limits, rubber hysteresis, multi-axis modes, and payload-dependent natural frequency.

Live graphs

About this model

A vibration isolator can be modeled as a single-degree-of-freedom mass-spring-damper system whose base moves harmonically. The displacement transmissibility T = X/Y compares absolute mass motion X to base motion Y and depends on frequency ratio r = ω/ω_n and damping ratio ζ. This simulator plots the standard base-excitation formula, animates the base and payload, and marks the isolation region where T < 1, which begins at r > √2 for displacement transmissibility. Damping is a tradeoff: it reduces the resonance peak near r = 1 but increases high-frequency leakage. The page omits nonlinear mounts, stroke limits, rubber hysteresis, multi-axis coupling, and payload-dependent natural-frequency shifts.

Who it's for: Machine dynamics, vibration control, mechanical design, and instrumentation mounting introductions.

Key terms

  • Transmissibility
  • Vibration isolation
  • Base excitation
  • Damping ratio
  • Frequency ratio

How it works

Single-degree-of-freedom vibration isolator under harmonic base excitation: compare mass motion to base motion and locate the isolation region above r = sqrt(2).

Key equations

T = X/Y = sqrt(1+(2ζr)^2) / sqrt((1-r²)^2+(2ζr)^2)
r = ω/ω_n; T < 1 for r > sqrt(2), but damping trades peak reduction for high-r leakage

Frequently asked questions

Why is r > sqrt(2) the isolation region?
For displacement transmissibility, the curve crosses T = 1 at r = √2. Above that frequency ratio the mass moves less than the base, so motion is isolated rather than amplified.
Is more damping always better?
No. Damping is valuable near resonance, where it limits the peak, but at high frequency it transmits more motion through the damper path.