# Exp8 - Exp#8 Acoustic Plane Waves 53 Exp#8 Acoustic Plane...

This preview shows pages 1–4. Sign up to view the full content.

53 Exp#8: Acoustic Plane Waves

This preview has intentionally blurred sections. Sign up to view the full version.

View Full Document
54 Exp#8: Acoustic Plane Waves 1. Properties of acoustic plane waves Acoustic waves are low amplitude pressure waves that propagate through a fluid according to the balance between inertia and compressibility. They are governed by the wave equation, 2 2 2 2 2 = t c x , ( 1 ) where is the fluctuating pressure, and c is a wave speed. Solutions to the sinusoidally-forced system have the form, ℘=℘ +℘ −+ A itk x B x ee () ωω , ( 2 ) which describes both forward (in + x direction) and backward moving waves with radian frequency , ω , and wavenumber, k = 2 π λ . ( 3 ) Since λ is the wavelength, k can be interpreted as the spatial equivalent of the radian frequency, ω . At any particular point in space and time, the wave phase, φ , is ω = tk x , ( 4 ) and if is fixed, then kx = t + C 1 , where C 1 is some constant phase offset. For convenience, let = 0, then C 1 = 0, kx = t , and c x == . ( 5 ) Similarly, from eq.(4) at fixed t (for example, t =0) then = kx , ( 6 ) and so ∂φ x k = . ( 7 ) k is the rate at which φ increases with x , and it is a constant. Note that eq.(7) is equivalent to eq.(3), where differences Δφ and x Δ are taken over one complete wave cycle. Acoustic plane waves are convenient theoretical objects, which vary and propagate in only one direction. It is possible to generate something like a plane wave by confining the acoustic disturbances to a cylindrical tube. If the wavelength, λ , is large compared to the tube diameter, if all reflected waves ( i.e. backward traveling components of eq.(2)) are small in amplitude compared to the forward traveling waves, and if boundary layer effects and viscous losses are ignored, then k can be measured by eq.(7) for a system forced at a known frequency, ω , when eq.(5) gives the speed of sound in air.
55 There is nothing in the wave equation that confines solutions to sines and cosines, and a more general solution to eq.(1) than eq.(2) is ℘ = + + fc t x gc () . ( 8 ) Once again, c is the wave speed, and f and g are unknown functions describing waves moving in positive and negative x respectively. 2. Generating and measuring sound waves While the fluid can, in principle, support wave motions with arbitrary shape (eq. 8), generating arbitrary pressure fluctuations is not so simple. The most common device for making sound waves is the loudspeaker, where fluctuations in voltage and current across a moving coil generate a force (through Maxwell’s equations) that moves the coil in one direction. The coil itself is attached to a cardboard cone of carefully-selected stiffness and suspension. Motion of the coil translates to motion of the cone, which imparts motion to the air next to it. Through the balance between inertia and compressibility, vibrations from the speaker propagate away at the speed of sound. All speakers represent a design compromise between small mass (rapid oscillations, high frequencies) and large size (large and uniform air volume displacements). They

This preview has intentionally blurred sections. Sign up to view the full version.

View Full Document
This is the end of the preview. Sign up to access the rest of the document.

## This note was uploaded on 10/12/2009 for the course AME 341AL at USC.

### Page1 / 6

Exp8 - Exp#8 Acoustic Plane Waves 53 Exp#8 Acoustic Plane...

This preview shows document pages 1 - 4. Sign up to view the full document.

View Full Document
Ask a homework question - tutors are online