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A soprano sings the note \(C 6(1046 \mathrm{~Hz})\) across the mouth of a soda bottle. To excite a fundamental frequency in the soda bottle equal to this note, describe how far the top of the liquid must be below the top of the bottle.

Short Answer

Expert verified
Answer: The liquid's surface should be placed 8.20 cm below the top of the bottle to excite a fundamental frequency equal to the sung note C6 (1046 Hz).

Step by step solution

01

Calculate the wavelength of the sound wave

To find the wavelength of the sound wave, we need to know the speed of sound in air. The speed of sound (\(v\)) is approximately \(343 \frac{m}{s}\) at room temperature. Given the frequency (\(f\)) of the sound wave, we can use the formula \(v = f\lambda\) to calculate the wavelength (\(\lambda\)) of the sound wave. Rearranging the formula for wavelength, \[\lambda = \frac{v}{f}\] We are given the frequency \(f = 1046 \mathrm{~Hz}\), and the speed of sound \(v = 343 \frac{m}{s}\). So, \[\lambda = \frac{343 \frac{\mathrm{m}}{\mathrm{s}}}{1046 \mathrm{~Hz}}\]
02

Calculate the wavelength of the sound wave

Now we substitute the given values of \(f\) and \(v\) in the formula, \[\lambda = \frac{343 \frac{\mathrm{m}}{\mathrm{s}}}{1046 \mathrm{~Hz}} \approx 0.3279 \mathrm{~m}\] This is the wavelength of the sound wave produced by the singing soprano.
03

Calculate the length of the air column in the bottle

To find the length of the air column inside the bottle that would resonate at this given frequency, we need to consider the fact that, for a closed-end air column, the length corresponds to one-fourth the wavelength. For an air column with one closed end (such as a bottle with liquid inside), the length (\(L\)) is given by: \[L = \frac{1}{4} \lambda\] Here, the length \(L\) is the distance from the top of the liquid to the top of the bottle. Now substitute the calculated wavelength value: \[L = \frac{1}{4} \cdot 0.3279 \mathrm{~m} \approx 0.0820 \mathrm{~m}\]
04

Convert the length to centimeters

Finally, we convert the calculated length of the air column in meters to centimeters for a more practical representation of the distance: \[L = 0.0820 \mathrm{~m} \cdot \frac{100 \mathrm{~cm}}{1 \mathrm{~m}} = 8.20 \mathrm{~cm}\] Thus, the liquid's surface should be \(8.20 \mathrm{~cm}\) below the top of the bottle in order to excite a fundamental frequency equal to the sung note \(C 6(1046 \mathrm{~Hz})\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Resonance
Resonance occurs when an object or system vibrates at a particular frequency with larger amplitude. This happens when the frequency of the externally applied vibrations matches the natural frequency of the system. In the context of acoustics, resonance is crucial to understanding how certain frequencies get amplified. For example, if a singer hits a note, the air inside a bottle can resonate and create a loud, clear sound if the frequency of the note matches the bottle's fundamental frequency. This is what happens in the described problem when a soprano sings a note across a soda bottle. The air column inside the bottle resonates at the frequency of the sung note if the lengths and conditions are just right, enhancing the sound as it reflects and builds upon itself within the bottle's confines.
Wavelength
Wavelength is the distance between successive crests of a wave, especially in sound or light. In acoustics, understanding wavelength is key to determining how waves behave in different environments. A wavelength (\(\lambda\)) is tied to both the speed of sound and the frequency of the wave through the equation:
  • \[ v = f\lambda \]
Where \(v\) is the speed of sound and \(f\) is the frequency. For the note \(C 6(1046\;\mathrm{Hz})\) sung across the soda bottle, the wavelength is calculated to be approximately \(0.3279\;\mathrm{m}\). This wavelength determines how the wave fits within the bottle and is essential for achieving resonance. By understanding the wavelength, you can predict the conditions needed for resonance in closed or open air columns.
Fundamental Frequency
The fundamental frequency is the lowest frequency at which a system naturally vibrates. In the case of the soda bottle, this is the frequency at which the air column vibrates when a minimal amount of energy is introduced. It is determined by the physical dimensions of the bottle and the characteristics of the air inside. For a bottle partially filled with liquid, the air column acts like a tube closed at one end, which means its fundamental frequency corresponds to a quarter of a wavelength fitting within the tube's length. This resonant frequency amplifies the sound at this pitch, which is precisely what the soprano is aiming to match with her singing.
Speed of Sound
The speed of sound is a measure of how quickly sound waves travel through a medium. It is affected by the medium itself (air, water, etc.) and also its temperature. For this exercise, sound travels through air at a speed of approximately \(343\;\frac{m}{s}\) at room temperature. Knowing the speed of sound is vital for calculating the wavelength of a sound wave and thus for determining the wavelengths and frequencies that will resonate in a given space. These concepts are interconnected and are essential to understanding how sound behaves in various conditions, including the resonance in a soda bottle when a specific note is sung across its mouth. The precise calculation of the sound speed assists in accurately predicting and achieving resonance.

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Most popular questions from this chapter

Standing on the sidewalk, you listen to the horn of a passing car. As the car passes, the frequency of the sound changes from high to low in a continuous manner; that is, there is no abrupt change in the perceived frequency. This occurs because a) the pitch of the sound of the horn changes continuously. b) the intensity of the observed sound changes continuously. c) you are not standing directly in the path of the moving car. d) of all of the above reasons.

A meteorite hits the surface of the ocean at a speed of \(8800 \mathrm{~m} / \mathrm{s}\). What are the shock wave angles it produces (a) in the air just before hitting the ocean surface, and (b) in the ocean just after entering? Assume the speed of sound in air and in water is \(343 \mathrm{~m} / \mathrm{s}\) and \(1560 \mathrm{~m} / \mathrm{s}\), respectively.

What has the greatest effect on the speed of sound in air? a) temperature of the air b) frequency of the sound c) wavelength of the sound d) pressure of the atmosphere

Two 100.0-W speakers, A and B, are separated by a distance \(D=3.6 \mathrm{~m} .\) The speakers emit in-phase sound waves at a frequency \(f=10,000.0 \mathrm{~Hz}\). Point \(P_{1}\) is located at \(x_{1}=4.50 \mathrm{~m}\) and \(y_{1}=0 \mathrm{~m} ;\) point \(P_{2}\) is located at \(x_{2}=4.50 \mathrm{~m}\) and \(y_{2}=-\Delta y .\) Neglecting speaker \(\mathrm{B}\), what is the intensity, \(I_{\mathrm{A} 1}\) (in \(\mathrm{W} / \mathrm{m}^{2}\) ), of the sound at point \(P_{1}\) due to speaker \(\mathrm{A}\) ? Assume that the sound from the speaker is emitted uniformly in all directions. What is this intensity in terms of decibels (sound level, \(\beta_{\mathrm{A} 1}\) )? When both speakers are turned on, there is a maximum in their combined intensities at \(P_{1} .\) As one moves toward \(P_{2},\) this intensity reaches a single minimum and then becomes maximized again at \(P_{2}\). How far is \(P_{2}\) from \(P_{1},\) that is, what is \(\Delta y ?\) You may assume that \(L \gg \Delta y\) and that \(D \gg \Delta y\), which will allow you to simplify the algebra by using \(\sqrt{a \pm b} \approx a^{1 / 2} \pm \frac{b}{2 a^{1 / 2}}\) when \(a \gg b\).

The Moon has no atmosphere. Is it possible to generate sound waves on the Moon?

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