Speed of sound

(notes by Roberto Bigoni)


Sound waves are compression waves in a gas.

If a mass of gas is steady and its density ρ0 is constant throughout the occupied volume, an explosion at a point S of the volume, after some time, causes the compression of a spherical shell centered on S.

After a short time, due to the elasticity of the gas, this shell returns to its equilibrium state and expands causing compression of the adjacent outer shell, and so on, so that the spherical compression moves away from the center with constant speed v.

boom.gif fig. 1

To understand how this speed depends on the characteristics of the gas, we ideally isolate a beam, ie a thin straight pipe of gas, which begins on the source S and is perpendicular to all the spherical shells.

fig. 2

In this beam, the area of compressed gas is represented by strata closer than in the unperturbed gas. If we assume that the compression propagates to the right with speed v, in a reference system fixed on the compressed zone, a point P on the right of the compressed zone moves towards the compressed zone with speed -v.

fig. 3

If we denote by ρ0 the density of the unperturbed gas and by A the section of the beam, the infinitesimal mass dm of gas in the volume of infinitesimal thickness dx is

Eqn001.gif

On the surface BC that separates a compressed stratum from an uncompressed one, for the second law of motion, acts a force of magnitude

Eqn002.gif

Since this force is opposed to speed, its relative expression is

Eqn003.gif

This force is equal to that produced by the pressure difference dp on both sides of the surface BC

Eqn004.gif

We obtain

Eqn005.gif

Furthermore, we have

Eqn006.gif

and then

Eqn007.gif

The expression on the right hand side, which is the opposite of the ratio between the variation of the pressure and the relative variation of the volume, is called the bulk modulus of the gas and is usually denoted by K.

Eqn008.gif

In conclusion, we obtain that the speed of the compression wave in the gas compression is given by

Eqn009.gif

Compressions and expansions of the gas strata are so fast that do not allow appreciable exchange of heat between one stratum and another and thus can be considered adiabatic processes. From the Poisson's law we have

Eqn010.gif

therefore

Eqn011.gif

Esempio

Considering the air as a diatomic ideal gas, we assume γ=1,4. At the pressure of one atmosphere (p ≅ 1,013·105Pa), the air has density ρ0 ≅ 1.225 kg/m3. The speed of sound is

Eqn012.gif

Conversely, by directly measuring the speed of sound, it is possible to obtain the value of γ by an alternative method to that of Clément-Desormes:

Eqn013.gif

Example

At the pressure of one atmosphere (p ≅ 1,013·105Pa), the air has density ρ0 ≅ 1.225 kg/m3. If a direct measurement of the speed of sound gives v = 344 m/s, then

Eqn014.gif


last revised October 23, 2015