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# Structural acoustics

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 Title: Structural acoustics Author: World Heritage Encyclopedia Language: English Subject: Collection: Publisher: World Heritage Encyclopedia Publication Date:

### Structural acoustics

Structural acoustics is the study of the mechanical waves in structures and how they interact with and radiate into adjacent media. The field of structural acoustics is often referred to as vibroacoustics in Europe and Asia. People that work in the field of structural acoustics are known as structural acousticians. The field of structural acoustics can be closely related to a number of other fields of acoustics including noise, transduction, underwater acoustics, and physical acoustics.

## Vibrations in Structures

### Compressional and Shear Waves (isotropic, homogeneous material)

Compressional waves (often referred to as longitudinal waves) expand and contract in the same direction (or opposite) as the wave motion. The wave equation dictates the motion of the wave in the x direction.

{ \partial^2 w \over \partial x ^2 } = {1 \over c_L^2} { \partial^2 w \over \partial t ^2 }

where w is the deformation c_L is the wave speed. This has the same form as the acoustic wave equation in one-dimension. c_L is determined by properties (bulk modulus B and density \rho) of the structure according to

{ c_L } = { \sqrt { B \over \rho } }

When two dimensions of the structure are small with respect to wavelength (commonly called a beam), the wave speed is dictated by Youngs modulus E instead of the B and are consequently slower than in infinite media.

Shear waves occur due to the shear stiffness and follows a similar equation, but with the shear deformation occurring in the transverse direction, perpendicular to the wave motion.

{ \partial^2 w \over \partial x ^2 } = {1 \over c_s^2} { \partial^2 w \over \partial t ^2 }

The shear wave speed is governed by the shear modulus G which is less than E and B, making shear waves slower than longitudinal waves.

### Bending Waves in beams and plates

Most sound radiation is caused by bending (or flexural) waves, which deform the structure transversely as they propagate. Bending waves are more complicated than compressional or shear waves and depend on material properties as well as geometric properties. They are also dispersive since different frequencies travel as different speeds. For a thin beam the bending wave speed is defined as

{ c_B } = { \left( { E I \omega^2 \over \rho A } \right)^{1 \over 4} }

and the wave equation is fourth order in space. For a thin plate the bending wave speed is

{ c_B } = { \left( { D \omega^2 \over \rho h } \right)^{1 \over 4} }

where {D}={E h^3 \over 12 ( 1 - \nu^2 ) }.

### Modeling Vibrations

Finite element analysis can be used to predict the vibration of complex structures. A finite element computer program will assemble the mass, stiffness, and damping matrices based on the element geometries and material properties, and solve for the vibration response based on the loads applied.

{ [ -\omega^2 \bold{M} + j \omega \bold{B} + (1 + j \eta ) \bold{K} ] } { \bold{d} = \bold{F} }

## Sound-Structure interaction

### Fluid-structure Interaction

When a vibrating structure is in contact with a fluid, the normal particle velocities at the interface must be conserved (i.e. be equivalent). This causes some of the energy from the structure to escape into the fluid, some of which radiates away as sound, some of which stays near the structure and does not radiate away.

A piston oscillating uniformly in a rigid baffle is the classic example to consider acoustic radiation. For a circular piston that has time harmonic motion, the pressure far away from the piston is found to be

{ p (r, \theta ) } = { j \omega \rho_0 a^2 v_n { J_1 (k a \sin \theta) \over k a \sin \theta } { e^{ j k r } \over r } }

where v_n is the piston velocity (assumed constant over the surface) and J_1 is the first order Bessel function. This is derived by integrating the far-field pressure contributions of tiny point sources over the area of the piston. The radiated sound power is related directly to the radiation resistance of the fluid and is calculated as

{ P_{rad} } = { R_0 <|v|>^2 }

where <|v|> is the spatially and time averaged velocity.