Compressibility Calculator

Calculate compressibility, bulk modulus, volume change, speed of sound, Mach number, and acoustic impedance for any material. Compare fluids, gases, and solids.

Material Presets

Use scientific notation e.g. 2.2e9
1 atm ≈ 101 325 Pa, 1 MPa = 1e6 Pa
Compressibility β
4.545 × 10^-10 Pa⁻¹
β = 1/K
Volume Change ΔV/V
-0.045455%
ΔV = -4.545 × 10^-4 m³
Speed of Sound
1,484.7 m/s
c = √(K/ρ)
Mach Number
0.0000
✅ Incompressible assumption OK
Density Change Δρ/ρ
0.045455%
New ρ = 998.454 kg/m³
Acoustic Impedance
1.482 × 10^6 Pa·s/m
Z = ρc
Strain Energy
227.27 J/m³
u = ΔP²/(2K)
Isothermal β (ideal gas)
9.869 × 10^-6 Pa⁻¹
βT = 1/P for ideal gas

Compressibility Spectrum

Material Comparison

MaterialK (GPa)ρ (kg/m³)c (m/s)β (Pa⁻¹)
Air (STP)0.00013407.042 × 10^-6
Water2.2009981,4854.545 × 10^-10
Seawater2.3401,0251,5114.274 × 10^-10
Engine Oil1.5008801,3066.667 × 10^-10
Glass40.0002,5004,0002.500 × 10^-11
Steel160.0007,8504,5156.250 × 10^-12
Diamond443.0003,51011,2342.257 × 10^-12

Volume Change vs Pressure

ΔP (MPa)ΔP (atm)ΔV/V (%)Δρ/ρ (%)
0.11.00.0045450.004545
19.90.0454550.045455
549.30.2272730.227273
1098.70.4545450.454545
50493.52.2727272.272727
100986.94.5454554.545455
5004,934.622.72727322.727273
10009,869.245.45454545.454545
Planning notes, formulas, and examples

About the Compressibility Calculator

The **Compressibility Calculator** determines how much a material's volume changes under pressure. Enter the bulk modulus, density, and applied pressure change, and the calculator returns the compressibility coefficient, fractional volume change, speed of sound, Mach number, density change, acoustic impedance, and strain energy density.

Compressibility is the reciprocal of the bulk modulus — a measure of a material's resistance to uniform compression. Gases are highly compressible; liquids are nearly incompressible; solids even less so. Understanding compressibility is critical in fluid mechanics (water hammer, hydraulic systems), acoustics (sound propagation), aerodynamics (shock waves above Mach 0.3), geophysics (seismic waves), and materials science.

Use the presets for water, air, steel, oil, seawater, and rubber, and refer to the materials comparison table to see how compressibility, sound speed, and acoustic impedance vary across orders of magnitude. Seeing those outputs together is useful when you need to decide whether the incompressible assumption is still reasonable for the material and pressure range you are using.

When This Page Helps

Use this page when you need to move from bulk modulus and density to practical outputs like volume change, sound speed, Mach number, and acoustic impedance. It is a quick way to connect a material property value to the flow, wave, or loading consequences that actually matter in design checks.

How to Use the Inputs

  1. Select a material preset or enter the bulk modulus in Pa.
  2. Enter the material density in kg/m³.
  3. Enter the ambient pressure and the applied pressure change in Pa.
  4. Enter the initial volume (for absolute ΔV).
  5. Optionally enter a flow speed for Mach number calculation.
  6. Read compressibility, volume change, sound speed, and related quantities.
Formula used
Compressibility: β = 1/K Volume Change: ΔV/V = −ΔP/K Speed of Sound: c = √(K/ρ) Mach Number: Ma = v/c Acoustic Impedance: Z = ρc Strain Energy: u = ΔP²/(2K)

Example Calculation

Result: β = 4.55×10⁻¹⁰ Pa⁻¹, ΔV/V = 0.045%, c = 1 484 m/s

Water has a bulk modulus of 2.2 GPa. A 1 MPa pressure increase compresses it by just 0.045% — effectively incompressible for most engineering purposes. Sound travels at 1 484 m/s.

Tips & Best Practices

  • Water is nearly incompressible: ΔV/V < 0.05% per MPa.
  • Air is ~15 000× more compressible than water at STP.
  • For aerodynamics, check Ma > 0.3 as the threshold for compressibility effects.
  • Acoustic impedance mismatch is why ultrasound gel is needed — air/tissue Z differs by ~4 000×.
  • Bulk modulus of seawater increases with depth (pressure), slightly increasing sound speed.

Compressibility In Practice

Compressibility links pressure loading to volume change. In gases that effect is obvious, but in liquids and solids it is small enough that many engineering models treat them as incompressible unless pressures become large or wave motion matters.

Why Sound Speed Appears Here

The same stiffness that resists compression also controls how fast pressure disturbances travel. That is why bulk modulus and density combine into the speed of sound and why compressibility shows up in acoustics, hydraulics, aerodynamics, and geophysics.

Model Limits

A single bulk modulus is often a simplification. Real materials can have temperature dependence, pressure dependence, or nonlinear behavior. Use the result as a first-pass property calculation unless you have a material-specific equation of state.

Sources & Methodology

Last updated:

Frequently Asked Questions

  • The fractional decrease in volume per unit increase in pressure. Higher compressibility means the material squeezes more easily under the same pressure change. Low compressibility means the same pressure produces only a small volume change.