# 17.5: Sound Interference and Resonance- Standing Waves in Air Columns

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- 1618

Interference is the hallmark of waves, all of which exhibit constructive and destructive interference exactly analogous to that seen for water waves. In fact, one way to prove something “is a wave” is to observe interference effects. So, sound being a wave, we expect it to exhibit interference; we have already mentioned a few such effects, such as the beats from two similar notes played simultaneously.

Figure \(\PageIndex{2}\) shows a clever use of sound interference to cancel noise. Larger-scale applications of active noise reduction by destructive interference are contemplated for entire passenger compartments in commercial aircraft. To obtain destructive interference, a fast electronic analysis is performed, and a second sound is introduced with its maxima and minima exactly reversed from the incoming noise. Sound waves in fluids are pressure waves and consistent with Pascal’s principle; pressures from two different sources add and subtract like simple numbers; that is, positive and negative gauge pressures add to a much smaller pressure, producing a lower-intensity sound. Although completely destructive interference is possible only under the simplest conditions, it is possible to reduce noise levels by 30 dB or more using this technique.

Where else can we observe sound interference? All sound resonances, such as in musical instruments, are due to constructive and destructive interference. Only the resonant frequencies interfere constructively to form standing waves, while others interfere destructively and are absent. From the toot made by blowing over a bottle, to the characteristic flavor of a violin’s sounding box, to the recognizability of a great singer’s voice, resonance and standing waves play a vital role.

Interference

Interference is such a fundamental aspect of waves that observing interference is proof that something is a wave. The wave nature of light was established by experiments showing interference. Similarly, when electrons scattered from crystals exhibited interference, their wave nature was confirmed to be exactly as predicted by symmetry with certain wave characteristics of light.

Suppose we hold a tuning fork near the end of a tube that is closed at the other end, as shown in Figure \(\PageIndex{3}\), Figure \(\PageIndex{4}\), Figure \(\PageIndex{5}\), and Figure \(\PageIndex{6}\). If the tuning fork has just the right frequency, the air column in the tube resonates loudly, but at most frequencies it vibrates very little. This observation just means that the air column has only certain natural frequencies. The figures show how a resonance at the lowest of these natural frequencies is formed. A disturbance travels down the tube at the speed of sound and bounces off the closed end. If the tube is just the right length, the reflected sound arrives back at the tuning fork exactly half a cycle later, and it interferes constructively with the continuing sound produced by the tuning fork. The incoming and reflected sounds form a standing wave in the tube as shown.

The standing wave formed in the tube has its maximum air displacement (an antinode) at the open end, where motion is unconstrained, and no displacement (a node) at the closed end, where air movement is halted. The distance from a node to an antinode is one-fourth of a wavelength, and this equals the length of the tube; thus, \(\lambda = 4L\). This same resonance can be produced by a vibration introduced at or near the closed end of the tube, as shown in Figure \(\PageIndex{7}\). It is best to consider this a natural vibration of the air column independently of how it is induced.

Given that maximum air displacements are possible at the open end and none at the closed end, there are other, shorter wavelengths that can resonate in the tube, such as the one shown in Figure \(\PageIndex{8}\). Here the standing wave has three-fourths of its wavelength in the tube, or \(L = (3/4) \lambda'\), so that \(\lambda' = 4L/3\). Continuing this process reveals a whole series of shorter-wavelength and higher-frequency sounds that resonate in the tube. We use specific terms for the resonances in any system. The lowest resonant frequency is called the **fundamental**, while all higher resonant frequencies are called **overtones**. All resonant frequencies are integral multiples of the fundamental, and they are collectively called **harmonics**. The fundamental is the first harmonic, the first overtone is the second harmonic, and so on. Figure \(\PageIndex{9}\)shows the fundamental and the first three overtones (the first four harmonics) in a tube closed at one end.

The fundamental and overtones can be present simultaneously in a variety of combinations. For example, middle C on a trumpet has a sound distinctively different from middle C on a clarinet, both instruments being modified versions of a tube closed at one end. The fundamental frequency is the same (and usually the most intense), but the overtones and their mix of intensities are different and subject to shading by the musician. This mix is what gives various musical instruments (and human voices) their distinctive characteristics, whether they have air columns, strings, sounding boxes, or drumheads. In fact, much of our speech is determined by shaping the cavity formed by the throat and mouth and positioning the tongue to adjust the fundamental and combination of overtones. Simple resonant cavities can be made to resonate with the sound of the vowels, for example. (See Figure \(\PageIndex{10}\).) In boys, at puberty, the larynx grows and the shape of the resonant cavity changes giving rise to the difference in predominant frequencies in speech between men and women.

Now let us look for a pattern in the resonant frequencies for a simple tube that is closed at one end. The fundamental has \(\lambda = 4L\), and frequency is related to wavelength and the speed of sound as given by:

\[v_w = f\lambda.\]

Solving for \(f\) in this equation gives

\[f = \dfrac{v_w}{\lambda} = \dfrac{v_w}{4L},\]

where \(v_w\) is the speed of sound in air. Similarly, the first overtone has \(\lambda' = 4L/3\) (see Figure \(\PageIndex{9}\)), so that

\[f' = 3\dfrac{v_w}{4L} = 3f.\]

Because \(f' = 3f\) we call the first overtone the third harmonic. Continuing this process, we see a pattern that can be generalized in a single expression. The resonant frequencies of a tube closed at one end are

\[f_n = n\dfrac{v_w}{4L}, \, n = 1, \, 3,\space 5,\]

where \(f_1\) is the fundamental, \(f_3\) is the first overtone, and so on. It is interesting that the resonant frequencies depend on the speed of sound and, hence, on temperature. This dependence poses a noticeable problem for organs in old unheated cathedrals, and it is also the reason why musicians commonly bring their wind instruments to room temperature before playing them.

Example\(\PageIndex{1}\): Find the Length of a Tube with a 128 Hz Fundamental

- What length should a tube closed at one end have on a day when the air temperature, is \(22^oC\), if its fundamental frequency is to be 128 Hz (C below middle C)?
- What is the frequency of its fourth overtone?

**Strategy**

The length \(L\) can be found from the relationship in \(f_n = n\frac{v_w}{4L}\), but we will first need to find the speed of sound \(v_w\).

**Solution for (a)**

(1) Identify knowns:

- the fundamental frequency is 128 Hz
- the air temperature is \(22^oC\)

(2) Use \(f_n = n\frac{v_w}{4L}\) to find the fundamental frequency (n = 1). \[f_1 = \dfrac{v_w}{4L}\]

(3) Solve this equation for length. \[L = \dfrac{v_w}{4f_1}\]

(4) Find the speed of sound using \(v_w = (331 \, m/s)\sqrt{\frac{T}{273 \, K}}\). \[v_w = (331 \, m/s)\sqrt{\dfrac{295 \, K}{273 \, K}} = 344 \, m/s\]

(5) Enter the values of the speed of sound and frequency into the expression for \(L\). \[L = \dfrac{v_w}{4f_1} = \dfrac{344 \, m/s}{4(128 \, Hz)} = 0.672 \, m\]

**Discussion on (a)**

Many wind instruments are modified tubes that have finger holes, valves, and other devices for changing the length of the resonating air column and hence, the frequency of the note played. Horns producing very low frequencies, such as tubas, require tubes so long that they are coiled into loops.

**Solution for (b)**

(1) Identify knowns:

- the first overtone has \(n = 3\)
- the second overtone has \(n = 5\)
- the third overtone has \(n = 7\)
- the fourth overtone has \(n = 9\)

(2) Enter the value for the fourth overtone into \(f_n = n\frac{v_w}{4L}\). \[f_9 = 9\dfrac{v_w}{4L} = 9f_1 = 1.15 \, kHz\]

**Discussion on (b)**

Whether this overtone occurs in a simple tube or a musical instrument depends on how it is stimulated to vibrate and the details of its shape. The trombone, for example, does not produce its fundamental frequency and only makes overtones.

Another type of tube is one that is *open* at both ends. Examples are some organ pipes, flutes, and oboes. The resonances of tubes open at both ends can be analyzed in a very similar fashion to those for tubes closed at one end. The air columns in tubes open at both ends have maximum air displacements at both ends, as illustrated in Figure \(\PageIndex{11}\). Standing waves form as shown.

Based on the fact that a tube open at both ends has maximum air displacements at both ends, and using Figure \(\PageIndex{11}\) as a guide, we can see that the resonant frequencies of a tube open at both ends are: \[f_n = n\dfrac{v_w}{2L}, \, n = 1, \, 2, \, 3...,\] where \(f_1\) is fundamental, \(f_2\) is the overtone, \(f_3\) is the second overtone, and so on. Note that a tube open at both ends has a fundamental frequency twice what it would have if closed at one end. It also has a different spectrum of overtones than a tube closed at one end. So if you had two tubes with the same fundamental frequency but one was open at both ends and the other was closed at one end, they would sound different when played because they have different overtones. Middle C, for example, would sound richer played on an open tube, because it has even multiples of the fundamental as well as odd. A closed tube has only odd multiples.

REAL WORLD APPLICATIONS: RESONANCE IN EVERYDAY

Resonance occurs in many different systems, including strings, air columns, and atoms. Resonance is the driven or forced oscillation of a system at its natural frequency. At resonance, energy is transferred rapidly to the oscillating system, and the amplitude of its oscillations grows until the system can no longer be described by Hooke’s law. An example of this is the distorted sound intentionally produced in certain types of rock music.

Wind instruments use resonance in air columns to amplify tones made by lips or vibrating reeds. Other instruments also use air resonance in clever ways to amplify sound. Figure \(\PageIndex{12}\)shows a violin and a guitar, both of which have sounding boxes but with different shapes, resulting in different overtone structures. The vibrating string creates a sound that resonates in the sounding box, greatly amplifying the sound and creating overtones that give the instrument its characteristic flavor. The more complex the shape of the sounding box, the greater its ability to resonate over a wide range of frequencies. The marimba, like the one shown in Figure \(\PageIndex{13}\)uses pots or gourds below the wooden slats to amplify their tones. The resonance of the pot can be adjusted by adding water.

We have emphasized sound applications in our discussions of resonance and standing waves, but these ideas apply to any system that has wave characteristics. Vibrating strings, for example, are actually resonating and have fundamentals and overtones similar to those for air columns. More subtle are the resonances in atoms due to the wave character of their electrons. Their orbitals can be viewed as standing waves, which have a fundamental (ground state) and overtones (excited states). It is fascinating that wave characteristics apply to such a wide range of physical systems.

Exercise \(\PageIndex{1}\)

Describe how noise-canceling headphones differ from standard headphones used to block outside sounds.

**Answer**-
Regular headphones only block sound waves with a physical barrier. Noise-canceling headphones use destructive interference to reduce the loudness of outside sounds.

Exercise \(\PageIndex{2}\)

How is it possible to use a standing wave's node and antinode to determine the length of a closed-end tube?

**Answer**-
When the tube resonates at its natural frequency, the wave's node is located at the closed end of the tube, and the antinode is located at the open end. The length of the tube is equal to one-fourth of the wavelength of this wave. Thus, if we know the wavelength of the wave, we can determine the length of the tube.

PHET EXPLORATIONS: SOUND

This simulation lets you see sound waves. Adjust the frequency or volume and you can see and hear how the wave changes. Move the listener around and hear what she hears.

## Summary

- Sound interference and resonance have the same properties as defined for all waves.
- In air columns, the lowest-frequency resonance is called the fundamental, whereas all higher resonant frequencies are called overtones. Collectively, they are called harmonics.
- The resonant frequencies of a tube closed at one end are: \(f_n = n\dfrac{v_w}{4L}, \, n = 1, \, 3, \, 5...,\) \(f_1\) is fundamental and \(L\) is the length of the tube.
- The resonant frequencies of a tube open at both ends are: \(f_n = n\dfrac{v_w}{2L}, \, n = 1, \, 2, \, 3...\)

## Glossary

**antinode**- point of maximum displacement

**node**- point of zero displacement

**fundamental**- the lowest-frequency resonance

**overtones**- all resonant frequencies higher than the fundamental

**harmonics**- the term used to refer collectively to the fundamental and its overtones

## Contributors and Attributions

Paul Peter Urone (Professor Emeritus at California State University, Sacramento) and Roger Hinrichs (State University of New York, College at Oswego) with Contributing Authors: Kim Dirks (University of Auckland) and Manjula Sharma (University of Sydney). This work is licensed by OpenStax University Physics under a Creative Commons Attribution License (by 4.0).