Audited 31 Jul 2026·Last updated 28 Oct 2026·3 citations·Tier 2·0 uses

Acoustic Impedance Calculator

Characteristic acoustic impedance Z = ρc in rayl from a material's density and sound speed, the number that sets how much sound reflects at a boundary.

Acoustic Impedance Calculator

kg/m³
m/s
Acoustic impedance
1,480,000
Characteristic acoustic impedance ρc in rayl (Pa·s/m); divide by one million for MRayl.
Model scope
Characteristic impedance for a homogeneous medium and longitudinal plane wave; frequency dependence, attenuation, complex impedance, boundaries, and oblique incidence are outside it.

Background.

Shout at someone swimming underwater and they will barely hear you. The sound is not soaked up by the water; almost all of it bounces off the surface, because air and water respond to the push of a sound wave in very different ways. That resistance to being set in motion is acoustic impedance, and the mismatch between two materials' impedances decides how much sound crosses the boundary between them and how much is turned back.

For a plane wave travelling through a uniform material, the impedance is simply density times sound speed, Z = ρc. Dense materials in which sound travels fast — steel, glass, bone — have high impedance; light, slow ones such as air have very little. Water comes out at about 1.48 million rayl and air at roughly 413, a ratio of around 3,600 to 1. At a flat surface hit head-on, that mismatch reflects about 99.9% of the sound energy: the swimming-pool problem in numbers.

The same arithmetic runs through a good deal of engineering. A medical ultrasound probe is used with gel because even a thin film of trapped air between transducer and skin would send nearly the whole pulse straight back. Ultrasonic flaw detection works because a crack, which is a thin layer of air inside metal, reflects strongly while sound metal lets the pulse through. Sonar and the matching layers bonded onto transducers are exercises in the same balancing act.

The result here is the characteristic impedance of one material. It assumes a homogeneous medium carrying a longitudinal plane wave, so it says nothing about frequency dependence, attenuation, the complex impedance of absorbent or layered materials, or waves meeting a boundary at an angle. To compare two materials, work out each one separately.

What is acoustic impedance calculator?

Characteristic acoustic impedance is the ratio of acoustic pressure to particle velocity in a plane sound wave travelling through a material. For a lossless homogeneous medium it equals density multiplied by sound speed, so it is a property of the material alone. Its SI unit is the pascal-second per metre, equivalent to kg/(m²·s) and called the rayl; values for liquids and solids are usually quoted in megarayl (MRayl), millions of rayl.

How to use this calculator.

  1. Enter the material's density in kilograms per cubic metre. Water is close to 1,000; for a gas, use the density at the actual temperature and pressure, since both change it substantially.
  2. Enter the longitudinal (compressional) sound speed in metres per second, taken at the same temperature as the density. For a solid, use the longitudinal value from a materials table, not the slower shear-wave speed.
  3. Read the impedance in rayl, and divide by one million to compare it with tables that quote MRayl.
  4. To estimate reflection at a boundary, work out the impedance of each material in turn and put the two results into the reflection formula given in the questions below.

The formula.

Z = ρc

Z = ρ × c, where ρ is the density in kg/m³ and c the longitudinal sound speed in m/s; the product has units of kg/(m²·s), the rayl. The relationship comes from the plane-wave solution of the linear acoustic equations. In such a wave the pressure p and the particle velocity u rise and fall together, with p = ρc × u, so ρc measures how much pressure it takes to drive the material's particles at a given speed. Both inputs enter to the first power, so doubling either doubles Z. Across everyday materials density varies far more than sound speed — air to steel is a factor of several thousand in density but under twenty in speed — which is why gases sit so far below liquids and solids. For a strongly absorbing material the impedance becomes a complex number that depends on frequency, and this simple product no longer describes it.

A worked example.

Example

Fresh water near room temperature has a density of about 1,000 kg/m³ and carries sound at about 1,480 m/s. Multiplying the two: Z = 1,000 × 1,480 = 1,480,000 rayl, or 1.48 MRayl. Air at 20 °C, at 1.204 kg/m³ and 343 m/s, gives 1.204 × 343 ≈ 413 rayl, about 3,580 times less. At a flat water surface the fraction of sound energy reflected, ((Z₂ − Z₁) ÷ (Z₂ + Z₁))², works out to 0.9989, so only about 0.11% gets through. Steel at roughly 7,850 kg/m³ and 5,900 m/s reaches about 46.3 MRayl, which means that even water against steel reflects about 88% of the incoming energy.

medium Density Kg M31,000
sound Speed Mps1,480

Frequently asked questions.

How do I work out how much sound reflects between two materials?
For a wave hitting a flat boundary head-on, the fraction of energy reflected is ((Z₂ − Z₁) ÷ (Z₂ + Z₁))², and the rest is transmitted. Equal impedances give no reflection at all; a large mismatch reflects almost everything. Water against air reflects about 99.9%, and water against steel about 88%.
Why does medical ultrasound need gel on the skin?
Without it, a thin layer of air would sit between the probe and the skin, and air's impedance is thousands of times lower than that of soft tissue, which is close to water's. Nearly the whole pulse would reflect at that gap. Water-based gel displaces the air so the sound can pass into the body.
What is a rayl, and why do some tables differ by a factor of ten?
The rayl, named after Lord Rayleigh, is the unit of specific acoustic impedance. In SI units one rayl is one pascal-second per metre. Older literature sometimes uses the CGS rayl, one dyne-second per cubic centimetre, which equals ten SI rayl, so check which one a table means before comparing values.
Should I enter the shear or the longitudinal sound speed for a solid?
The longitudinal speed, because the page describes compressional plane waves. Solids also carry shear waves, which travel more slowly and have their own impedance based on the shear speed. Ultrasonic testing with angled shear-wave probes needs that second figure, which this page does not compute.
Is this the same acoustic impedance used for pipes and loudspeaker enclosures?
Not quite. Duct and enclosure work often uses pressure divided by volume velocity, in pascal-seconds per cubic metre. For a plane wave in a duct of cross-sectional area S, that quantity equals ρc ÷ S. The value here is the specific, per-unit-area version that describes the material itself.
Does temperature change acoustic impedance?
Yes, through both density and sound speed. In air at constant pressure, warming lowers the density in proportion to absolute temperature while raising the sound speed only with its square root, so impedance falls slightly as air warms. Enter density and speed measured at the same temperature to keep the two consistent.

How this page was produced

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Quanta Calculator
Primary sources
3 cited below
Method
Z = ρc
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