/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 59 A soprano and a bass are singing... [FREE SOLUTION] | 91Ó°ÊÓ

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A soprano and a bass are singing a duet. While the soprano sings an A-sharp at 932 Hz, the bass sings an A-sharp but three octaves lower. In this concert hall, the density of air is 1.20 kg/m\(^3\) and its bulk modulus is 1.42 \(\times\) 10\(^5\) Pa. In order for their notes to have the same sound intensity level, what must be (a) the ratio of the pressure amplitude of the bass to that of the soprano and (b) the ratio of the displacement amplitude of the bass to that of the soprano? (c) What displacement amplitude (in m and in nm) does the soprano produce to sing her A-sharp at 72.0 dB?

Short Answer

Expert verified
The ratio of pressure amplitudes is \(2^{-3/2}\) and the displacement amplitude ratio is \(2^{3/2}\). Soprano's displacement amplitude is approximately \(2.5 \times 10^{-9}\) m or \(2.5\) nm.

Step by step solution

01

Understanding the Frequency Relationship

The frequency of a note decreases by half for each octave that is lowered. The soprano sings at 932 Hz. Since the bass is singing three octaves lower, his frequency is: \(932 \text{ Hz} / 2^3 = 932 \text{ Hz} / 8 = 116.5 \text{ Hz}\).
02

Calculate the Sound Intensity Level Conversion

The sound intensity level \(L\) in decibels is given by \(L = 10 \log_{10}(\frac{I}{I_0})\), where \(I_0 = 10^{-12} \text{ W/m}^2\) is the reference intensity. For \(L = 72 \text{ dB}\), the intensity \(I\) is \(I_0 \times 10^{7.2} = 10^{-12} \times 10^{7.2}\).
03

Calculate Pressure Amplitude Ratio

Pressure amplitude \(p_0\) is related to intensity by \(p_0 = \sqrt{2 \rho c I}\), where \(\rho\) is the density of air and \(c\) is the speed of sound in air given by \(c = \sqrt{\frac{B}{\rho}}\). For both soprano and bass, \(c\) remains the same, thus the ratio of pressure amplitudes \(\frac{p_{0, \text{bass}}}{p_{0, \text{soprano}}} = \sqrt{\frac{f_\text{bass}}{f_\text{soprano}}}\).
04

Calculate Displacement Amplitude Ratio

Displacement amplitude \(s_0\) is related to the pressure amplitude by \(s_0 = \frac{p_0}{\omega \rho c}\), where \(\omega\) is the angular frequency. Therefore, the ratio of displacement amplitudes is \(\frac{s_{0, \text{bass}}}{s_{0, \text{soprano}}} = \frac{f_\text{soprano}}{f_\text{bass}} \times \frac{p_{0, \text{bass}}}{p_{0, \text{soprano}}}\).
05

Calculate Soprano's Displacement Amplitude

Given the intensity, we can find the pressure amplitude for the soprano using \(p_{0, \text{soprano}} = \sqrt{2 \rho c I}\). Then, using \(s_0 = \frac{p_0}{\omega \rho c}\) with \(\omega = 2 \pi f\), we find the displacement amplitude in meters and convert it to nanometers (1 m = 10^9 nm).
06

Final Calculations and Units Conversion

After calculating the soprano's pressure amplitude, substitute it to find the displacement amplitude \(s_{0, \text{soprano}}\). Convert the result from meters to nanometers for convenient representation.

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Key Concepts

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

Frequency Relationship
The concept of frequency relationship is vital when comparing sounds, especially in the context of octaves. An octave is a musical interval where one note has a frequency that is double or half the frequency of another. For example, if a soprano sings an A-sharp at 932 Hz, a note three octaves lower would be found by continuously halving the frequency. This is calculated as follows: - First octave lower: 932 Hz / 2 = 466 Hz - Second octave lower: 466 Hz / 2 = 233 Hz - Third octave lower: 233 Hz / 2 = 116.5 Hz Therefore, the bass's A-sharp is at 116.5 Hz. Understanding this frequency relationship helps us comprehend the idea of musical intervals and changes in tone.
Sound Intensity Level
Sound intensity level, measured in decibels (dB), quantifies how loud a sound is. The formula to calculate it is:\[ L = 10 \log_{10} \left( \frac{I}{I_0} \right) \]where:- \( L \) is the sound intensity level,- \( I \) is the sound intensity, and- \( I_0 \) is the reference intensity, typically \( 10^{-12} \text{ W/m}^2 \).In our scenario, the soprano sings at 72 dB. This means:\[ I = I_0 \times 10^{7.2} \]Calculating sound intensity helps in understanding the variation of loudness perceived by the human ear with varying sound intensities.
Pressure Amplitude
Pressure amplitude \( p_0 \) represents the maximum change in pressure from the sound wave. It's particularly important when comparing different sound sources, like a soprano's and a bass's notes.We use the formula:\[ p_0 = \sqrt{2 \rho c I} \]- \( \rho \) is the air density (1.20 kg/m\(^3\) here),- \( c \) is the speed of sound, - \( I \) is the sound intensity.In our case, since the soprano's and bass's notes are played in the same environment, the speed of sound \( c \) remains constant. The formula for the pressure amplitude ratio between bass and soprano becomes:\[ \frac{p_{0, \text{bass}}}{p_{0, \text{soprano}}} = \sqrt{\frac{f_{\text{bass}}}{f_{\text{soprano}}}} \]This ratio is fundamental in understanding the relative pressure changes generated by each singer's voice.
Displacement Amplitude
Displacement amplitude \( s_0 \) describes how far air particles move during a sound wave. It depends on pressure amplitude, frequency, and the medium's properties.The formula is:\[ s_0 = \frac{p_0}{\omega \rho c} \]where:- \( \omega \) is the angular frequency (\( 2 \pi f \)), - \( p_0 \) is the pressure amplitude,- \( \rho \) is air density,- \( c \) is the speed of sound.To find the displacement amplitude ratio between the bass and the soprano:\[ \frac{s_{0, \text{bass}}}{s_{0, \text{soprano}}} = \frac{f_{\text{soprano}}}{f_{\text{bass}}} \times \frac{p_{0, \text{bass}}}{p_{0, \text{soprano}}} \]This ratio lets us compare how much the air particles are displaced by each sound, offering insight into the physical effect of each singer's note.
Octave
An octave is a fundamental concept in music theory, representing a doubling or halving of frequency. It's key in understanding scales and harmony. When a note is one octave higher, its frequency is double that of the original note. Conversely, if it is one octave lower, the frequency is halved. In musical practice, this relationship maintains the note's identity while altering its pitch height. In the current exercise, the bass sings three octaves lower than the soprano. This means his note's frequency is half of the soprano's frequency, three times over. The idea of octaves helps musicians and sound engineers adjust notes within scales and matches the resonance to desired musical keys. It's crucial for modulating sound and comprehending how frequency affects pitch perception.

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Most popular questions from this chapter

(a) A sound source producing 1.00-kHz waves moves toward a stationary listener at one-half the speed of sound. What frequency will the listener hear? (b) Suppose instead that the source is stationary and the listener moves toward the source at one-half the speed of sound. What frequency does the listener hear? How does your answer compare to that in part (a)? Explain on physical grounds why the two answers differ.

Standing sound waves are produced in a pipe that is 1.20 m long. For the fundamental and first two overtones, determine the locations along the pipe (measured from the left end) of the displacement nodes and the pressure nodes if (a) the pipe is open at both ends and (b) the pipe is closed at the left end and open at the right end.

Horseshoe bats (genus \(Rhinolophus\)) emit sounds from their nostrils and then listen to the frequency of the sound reflected from their prey to determine the prey's speed. (The "horseshoe" that gives the bat its name is a depression around the nostrils that acts like a focusing mirror, so that the bat emits sound in a narrow beam like a flashlight.) A \(Rhinolophus\) flying at speed \(v_{bat}\) emits sound of frequency \(f_{bat}\); the sound it hears reflected from an insect flying toward it has a higher frequency \(f_{refl}\). (a) Show that the speed of the insect is $$vinsect = v\Bigg[\frac{f_{refl}(v - v_{bat}) - f_{bat}(v + v_{bat})}{f_{refl}(v - v_{bat}) + f_{bat}(v + v_{bat})}\Bigg] $$ where \(v\) is the speed of sound. (b) If \(f_{bat} =\) 80.7 kHz, \(f_{refl} =\) 83.5 kHz, and \(v_{bat} =\) 3.9 m/s, calculate the speed of the insect.

What must be the stress \((F/A)\) in a stretched wire of a material whose Young's modulus is \(Y\) for the speed of longitudinal waves to equal 30 times the speed of transverse waves?

A loud factory machine produces sound having a displacement amplitude of 1.00 \(\mu\)m, but the frequency of this sound can be adjusted. In order to prevent ear damage to the workers, the maximum pressure amplitude of the sound waves is limited to 10.0 Pa. Under the conditions of this factory, the bulk modulus of air is 1.42 \(\times\) 10\(^5\) Pa. What is the highest-frequency sound to which this machine can be adjusted without exceeding the prescribed limit? Is this frequency audible to the workers?

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