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There are other numerous examples of resonance in standing waves in the physical world. The air in a tube, such as found in a musical instrument like a flute, can be forced into resonance and produce a pleasant sound, as we discuss in Sound .

At other times, resonance    can cause serious problems. A closer look at earthquakes provides evidence for conditions appropriate for resonance, standing waves, and constructive and destructive interference. A building may vibrate for several seconds with a driving frequency matching that of the natural frequency of vibration of the building—producing a resonance resulting in one building collapsing while neighboring buildings do not. Often, buildings of a certain height are devastated while other taller buildings remain intact. The building height matches the condition for setting up a standing wave for that particular height. The span of the roof is also important. Often it is seen that gymnasiums, supermarkets, and churches suffer damage when individual homes suffer far less damage. The roofs with large surface areas supported only at the edges resonate at the frequencies of the earthquakes, causing them to collapse. As the earthquake waves travel along the surface of Earth and reflect off denser rocks, constructive interference occurs at certain points. Often areas closer to the epicenter are not damaged, while areas farther away are damaged.

Summary

  • A standing wave is the superposition of two waves which produces a wave that varies in amplitude but does not propagate.
  • Nodes are points of no motion in standing waves.
  • An antinode is the location of maximum amplitude of a standing wave.
  • Normal modes of a wave on a string are the possible standing wave patterns. The lowest frequency that will produce a standing wave is known as the fundamental frequency. The higher frequencies which produce standing waves are called overtones.

Key equations

Wave speed v = λ T = λ f
Linear mass density μ = mass of the string length of the string
Speed of a wave or pulse on a string under
tension
| v | = F T μ
Speed of a compression wave in a fluid v = Β ρ
Resultant wave from superposition of two
sinusoidal waves that are identical except for a
phase shift
y R ( x , t ) = [ 2 A cos ( ϕ 2 ) ] sin ( k x ω t + ϕ 2 )
Wave number k 2 π λ
Wave speed v = ω k
A periodic wave y ( x , t ) = A sin ( k x ω t + ϕ )
Phase of a wave k x ω t + ϕ
The linear wave equation 2 y ( x , t ) x 2 = 1 v w 2 2 y ( x , t ) t 2
Power in a wave for one wavelength P ave = E λ T = 1 2 μ A 2 ω 2 λ T = 1 2 μ A 2 ω 2 v
Intensity I = P A
Intensity for a spherical wave I = P 4 π r 2
Equation of a standing wave y ( x , t ) = [ 2 A sin ( k x ) ] cos ( ω t )
Wavelength for symmetric boundary
conditions
λ n = 2 n L , n = 1 , 2 , 3 , 4 , 5 ...
Frequency for symmetric boundary conditions f n = n v 2 L = n f 1 , n = 1 , 2 , 3 , 4 , 5 ...

Conceptual questions

A truck manufacturer finds that a strut in the engine is failing prematurely. A sound engineer determines that the strut resonates at the frequency of the engine and suspects that this could be the problem. What are two possible characteristics of the strut can be modified to correct the problem?

It may be as easy as changing the length and/or the density a small amount so that the parts do not resonate at the frequency of the motor.

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Source:  OpenStax, University physics volume 1. OpenStax CNX. Sep 19, 2016 Download for free at http://cnx.org/content/col12031/1.5
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