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BIO For a person with normal hearing, the faintest sound that can be heard at a frequency of 400 \(\mathrm{Hz}\) has a pressure amplitude of about \(6.0 \times 10^{-5}\) Pa. Calculate the (a) intensity; (b) sound intensity level; (c) displacement amplitude of this sound wave at \(20^{\circ} \mathrm{C} .\)

Short Answer

Expert verified
(a) 3.0 × 10^-12 W/m^2; (b) 4.77 dB; (c) 5.81 × 10^-11 m.

Step by step solution

01

Calculate Sound Intensity

The intensity of a sound wave is calculated using the formula \(I = \frac{p^2}{2 \rho v}\), where \(p\) is the pressure amplitude, \(\rho\) is the density of air, and \(v\) is the speed of sound in air at the given temperature. At \(20^{\circ}\)C, \(\rho \approx 1.2041 \, \text{kg/m}^3\) and \(v \approx 343 \, \text{m/s}\). Substitute the given pressure amplitude \(p = 6.0 \times 10^{-5} \, \text{Pa}\). \[I = \frac{(6.0 \times 10^{-5})^2}{2 \times 1.2041 \times 343} \approx 3.0 \times 10^{-12} \, \text{W/m}^2\]
02

Calculate Sound Intensity Level

The sound intensity level \(L\) is calculated using the formula \(L = 10 \log_{10} \left( \frac{I}{I_0} \right)\), where \(I_0 = 10^{-12} \, \text{W/m}^2\) is the reference intensity. Substitute the calculated intensity \(I = 3.0 \times 10^{-12} \, \text{W/m}^2\). \[L = 10 \log_{10} \left( \frac{3.0 \times 10^{-12}}{10^{-12}} \right) \approx 4.77 \, \text{dB}\]
03

Calculate Displacement Amplitude

The displacement amplitude \(A\) of the sound wave can be found using \(A = \frac{p}{\omega Z}\), where \(\omega = 2 \pi f\) is the angular frequency and \(Z = \rho v\) is the acoustic impedance. \(f = 400 \, \text{Hz}\). First, calculate \(\omega\) and \(Z\): \(\omega = 2 \pi \times 400 \approx 2513.27\) and \(Z = 1.2041 \times 343 \approx 413.01\). Then \[A = \frac{6.0 \times 10^{-5}}{2513.27 \times 413.01} \approx 5.81 \times 10^{-11} \, \text{m}\]

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Key Concepts

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

Pressure Amplitude
Pressure amplitude is a measure of the maximum change in pressure caused by a sound wave as it travels through a medium. It indicates how compressed or rarefied the medium becomes with the passing of the wave.
Understanding pressure amplitude is crucial because it relates to the physical sensation of loudness—a higher pressure amplitude typically means a louder sound.
  • Pressure amplitude is measured in Pascals (Pa).
  • It is a peak value, representing the furthest extent of compression or rarefaction of the air particles.
  • In the exercise provided, the pressure amplitude of the sound is given as approximately \(6.0 \times 10^{-5}\) Pa.
This value tells us about the faintest sound a person with normal hearing can detect at a particular frequency. A small change in this amplitude can mean a significant difference in perceived loudness.
Sound Intensity Level
Sound intensity level is a logarithmic measure of the intensity of sound. It gives us a sense of how loud a sound appears to be in comparison to a standard reference point.
This concept is very useful because it scales vast intensity ranges into manageable numbers, typically measured in decibels (dB).
  • The formula used is \(L = 10 \log_{10} \left( \frac{I}{I_0} \right)\), where \(I\) is the intensity of the sound, and \(I_0 = 10^{-12} \, \text{W/m}^2\) is the reference intensity, which is typically the threshold of hearing.
  • In our case, the calculated sound intensity level is approximately 4.77 dB.
  • This level tells us how the sound compares to the quietest sound perceivable by the average human ear.
The scale is logarithmic, meaning every increase of 10 dB represents a tenfold increase in intensity.
Displacement Amplitude
The displacement amplitude refers to the maximum distance that particles in a medium are displaced from their resting positions due to the passage of a sound wave. It captures the actual movement of particles as the wave energy propagates through the medium.
For sound waves, this is fundamental in understanding how sound travels through materials.
  • The relationship between pressure and displacement can be described by the equation \(A = \frac{p}{\omega Z}\), where \(A\) is displacement amplitude, \(p\) is the pressure amplitude, \(\omega\) is the angular frequency, and \(Z\) is the acoustic impedance.
  • For the given example, the displacement amplitude is approximately \(5.81 \times 10^{-11}\) m, indicating very slight movements of the particles at the sound's stated intensity.
  • This concept is instrumental in fields like acoustics, helping to design better soundproofing and understand wave interactions with different materials.
Angular Frequency
Angular frequency relates to how quickly a wave oscillates in terms of radians per second. It is essential in connecting circular motion concepts to wave phenomena.
In the context of sound waves, it helps characterize the wave’s energy and behavior.
  • Calculated using the formula \(\omega = 2 \pi f\), where \(f\) is the frequency of the wave.
  • For instance, in our given problem, \(f = 400 \, \text{Hz}\), making \(\omega \approx 2513.27\, \text{radians/second}\).
  • Higher angular frequencies indicate more rapid vibrations, contributing to higher pitch sounds.
Angular frequency is connected to how we perceive sound and is directly proportional to both the velocity and distance properties of waves.
Acoustic Impedance
Acoustic impedance is a measure of resistance a medium offers to the propagation of sound waves. It connects the sound pressure with particle velocity in the medium and is pivotal in studying sound transmission and reflection.
The concept is akin to electrical impedance but applied to sound waves.
  • Defined as \(Z = \rho v\), where \(\rho\) is the density of the medium and \(v\) is the speed of sound within it.
  • In the given example, considering the air at approximately \(20^{\circ} \mathrm{C}\), \(Z \approx 413.01\, \text{kg/(m}^2\cdot \text{s)}\).
  • Acoustic impedance influences how sound waves travel through different media, determining how much energy is reflected or absorbed upon hitting a surface. This is crucial for engineering fields like audio technology and architectural acoustics.
Understanding acoustic impedance aids in the design of audio systems and sound isolation techniques.

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Most popular questions from this chapter

BIO Ultrasound in Medicine. A \(2.00-\) MHz sound wave travels through a pregnant woman's abdomen and is reflected from the fetal heart wall of her unborn baby. The heart wall is moving toward the sound receiver as the heart beals. The reflected sound is then mixed with the transmitted sound, and 72 beats per second are detected. The speed of sound in body tissue is 1500 \(\mathrm{m} / \mathrm{s}\) . Calculate the speed of the fetal heart wall at the instant this measurement is made.

A sound wave in air at \(20^{\circ} \mathrm{C}\) has a frequency of 150 \(\mathrm{Hz}\) and a displacement amplitude of \(5.00 \times 10^{-3} \mathrm{mm} .\) For this sound wave calculate the (a) pressure amplitude (in \(\mathrm{Pa} ) ;\) (b) intensity (in \(\mathrm{W} / \mathrm{m}^{2} ) ;(\mathrm{c})\) sound intensity level (in decibels).

A swimming duck paddles the water with its feet once every 1.6 \(\mathrm{s}\) , producing surface waves with this period. The duck is moving at constant speed in a pond where the speed of surface waves is \(0.32 \mathrm{m} / \mathrm{s},\) and the crests of the waves ahead of the duck are spaced 0.12 \(\mathrm{m}\) apart. (a) What is the duck's speed? (b) How far apart are the crests behind the duck's.

The shock-wave cone created by the space shuttle at one instant during its reentry into the atmosphere makes an angle of \(58.0^{\circ}\) with its direction of motion. The speed of sound at this altitude is 331 \(\mathrm{m} / \mathrm{s}\) . (a) What is the Mach number of the shuttle at this instant, and (b) how fast (in \(\mathrm{m} / \mathrm{s}\) and in \(\mathrm{mi} / \mathrm{h} )\) is it traveling relative to the atmosphere? (c) What would be its Mach number and the angle of its shock-wave cone if it flew at the same speed but at low altitude where the speed of sound is 344 \(\mathrm{m} / \mathrm{s} ?\)

Wagnerian Opera. A man marries a great Wagnerian soprano but, alas, he discovers he cannot stand Wagnerian opera. In order to save his eardrums, the unhappy man decides he must silence his larklike wife for good. His plan is to tie her to the front of his car and send car and soprano speeding toward a brick wall. This soprano is quite shrewd, however, having studied physics in her student days at the music conservatory. She realizes that this wall has a resonant frequency of 600 \(\mathrm{Hz}\) , which means that if a continuous sound wave of this frequency hits the wall, it will fall down, and she will be saved to sing more Isoldes. The car is heading toward the wall at a high speed of 30 \(\mathrm{m} / \mathrm{s}\) . (a) At what frequency must the soprano sing so that the will will crumble? (b) What frequency will the soprano hear reflected from the wall just before it crumbles?

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