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Acoustic theory

From Wikipedia, the free encyclopedia

Acoustic theory is a scientific field that relates to the description of sound waves. It derives from fluid dynamics. See acoustics for the engineering approach.

For sound waves of any magnitude of a disturbance in velocity, pressure, and density we have

In the case that the fluctuations in velocity, density, and pressure are small, we can approximate these as

Where is the perturbed velocity of the fluid, is the pressure of the fluid at rest, is the perturbed pressure of the system as a function of space and time, is the density of the fluid at rest, and is the variance in the density of the fluid over space and time.

In the case that the velocity is irrotational (), we then have the acoustic wave equation that describes the system:

Where we have


Derivation for a medium at rest

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Starting with the Continuity Equation and the Euler Equation:

If we take small perturbations of a constant pressure and density:

Then the equations of the system are

Noting that the equilibrium pressures and densities are constant, this simplifies to

A Moving Medium

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Starting with

We can have these equations work for a moving medium by setting , where is the constant velocity that the whole fluid is moving at before being disturbed (equivalent to a moving observer) and is the fluid velocity.

In this case the equations look very similar:

Note that setting returns the equations at rest.

Linearized Waves

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Starting with the above given equations of motion for a medium at rest:

Let us now take to all be small quantities.

In the case that we keep terms to first order, for the continuity equation, we have the term going to 0. This similarly applies for the density perturbation times the time derivative of the velocity. Moreover, the spatial components of the material derivative go to 0. We thus have, upon rearranging the equilibrium density:

Next, given that our sound wave occurs in an ideal fluid, the motion is adiabatic, and then we can relate the small change in the pressure to the small change in the density by

Under this condition, we see that we now have

Defining the speed of sound of the system:

Everything becomes

For Irrotational Fluids

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In the case that the fluid is irrotational, that is , we can then write and thus write our equations of motion as

The second equation tells us that

And the use of this equation in the continuity equation tells us that

This simplifies to

Thus the velocity potential obeys the wave equation in the limit of small disturbances. The boundary conditions required to solve for the potential come from the fact that the velocity of the fluid must be 0 normal to the fixed surfaces of the system.

Taking the time derivative of this wave equation and multiplying all sides by the unperturbed density, and then using the fact that tells us that

Similarly, we saw that . Thus we can multiply the above equation appropriately and see that

Thus, the velocity potential, pressure, and density all obey the wave equation. Moreover, we only need to solve one such equation to determine all other three. In particular, we have

For a moving medium

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Again, we can derive the small-disturbance limit for sound waves in a moving medium. Again, starting with

We can linearize these into

For Irrotational Fluids in a Moving Medium

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Given that we saw that

If we make the previous assumptions of the fluid being ideal and the velocity being irrotational, then we have

Under these assumptions, our linearized sound equations become

Importantly, since is a constant, we have , and then the second equation tells us that

Or just that

Now, when we use this relation with the fact that , alongside cancelling and rearranging terms, we arrive at

We can write this in a familiar form as

This differential equation must be solved with the appropriate boundary conditions. Note that setting returns us the wave equation. Regardless, upon solving this equation for a moving medium, we then have

See also

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References

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  • Landau, L.D.; Lifshitz, E.M. (1984). Fluid Mechanics (2nd ed.). Butterworth-Heinenann. ISBN 0-7506-2767-0.
  • Fetter, Alexander; Walecka, John (2003). Fluid Mechanics (1st ed.). Courier Corporation. ISBN 0-486-43261-0.