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Introduction to Acoustics

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212 Part B Physical and Nonlinear <strong>Acoustics</strong><br />

Part B 6.1<br />

reflection coefficient given by<br />

�2 Z2 + Z1<br />

, (6.7)<br />

�<br />

Z2 − Z1<br />

R =<br />

where Z1 and Z2 are the impedances of the two media.<br />

Since both values of Z must be positive, R must be less<br />

than one. The fraction of the energy transmitted in<strong>to</strong> the<br />

second medium is given by T = 1 − R because 100% of<br />

the energy must be divided between T and R.<br />

Refraction<br />

Refraction is a change of the direction of wave propagation<br />

as the wave passes from one medium in<strong>to</strong> another<br />

across an interface. Bending occurs when the wave speed<br />

is different in the two media. If there is an angle between<br />

the normal <strong>to</strong> the plane of the boundary and the incident<br />

wave, there is a brief time interval when part of the wave<br />

is in the original medium (traveling at one velocity) and<br />

part of the wave is in the second medium (traveling<br />

at a different velocity). This causes the bending of the<br />

waves as they pass from the first medium <strong>to</strong> the second.<br />

(There is no bending at normal incidence.)<br />

Reflection and refraction can occur simultaneously<br />

when a wave impinges on a boundary between two<br />

media with different wave propagation speeds. Some<br />

of the energy of the wave is reflected back in<strong>to</strong> the<br />

original medium, and some of the energy is transmitted<br />

and refracted in<strong>to</strong> the second medium. This<br />

means that a wave incident on a boundary can generate<br />

two waves: a reflected wave and a transmitted<br />

wave whose direction of propagation is determined by<br />

Snell’s law.<br />

a) b)<br />

Wave velocity<br />

Waves are here but<br />

transverse particle motion<br />

is suppressed<br />

Waves pass through each other<br />

and continue propagating<br />

Wave velocity<br />

Wave velocity<br />

Wave velocity<br />

Destructive<br />

interference<br />

All waves obey Snell’s law. For optical waves the<br />

proper form of Snell’s law is:<br />

n1 sin θ1 = n2 sin θ2 , (6.8)<br />

where n1 and n2 are the refractive indices and θ1 and<br />

θ2 are propagation directions. For acoustic waves the<br />

proper form of Snell’s law is:<br />

sin θ1<br />

= sin θ2<br />

Wave velocity Wave velocity<br />

Addition of<br />

wave amplitudes<br />

Waves pass through each other<br />

and continue propagating<br />

Wave velocity<br />

Wave velocity<br />

Fig. 6.6a,b Two waves passing through each other exhibiting (a) destructive and (b) constructive interference<br />

v1<br />

, (6.9)<br />

v2<br />

where v1 is the wave velocity in medium 1 and v2 is the<br />

wave velocity in medium 2. These two forms are very<br />

similar since the refractive index is n = c/Cm,wherec is<br />

the velocity of light in a vacuum and Cm is the velocity<br />

of light in the medium under consideration.<br />

Interference<br />

Spatial Interference. Interference is a phenomenon that<br />

occurs when two (or more) waves add <strong>to</strong>gether. Consider<br />

two identical transverse waves traveling <strong>to</strong> the right<br />

(one after the other) down a string <strong>to</strong>wards a boundary<br />

at the end. When the first wave encounters the<br />

boundary, it reflects and travels in the leftward direction.<br />

When it encounters the second, rightward moving<br />

wave the two waves add <strong>to</strong>gether linearly (in accordance<br />

with the principle of superposition). The displacement<br />

amplitude at the point in space where two waves combine<br />

is either greater than or less than the displacement<br />

amplitude of each wave. If the resultant wave has an<br />

amplitude that is smaller than that of either of the<br />

original two waves, the two waves are said <strong>to</strong> have<br />

Constructive<br />

interference

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