(a) What is the intensity in watts per meter squared of a just barely audible \({\rm{200 Hz}}\) sound? (b) What is the intensity in watts per meter squared of a barely audible \({\rm{4000 Hz}}\) sound?

Short Answer

Expert verified

(a) Intensity of a just barely audible \(200{\rm{ }}Hz\) sound will be \(1.3 \times {10^{ - 10}}{\rm{ }}W \cdot {m^{ - 2}}\).

(b) Intensity of a just barely audible \(4000{\rm{ }}Hz\) sound will be \(2 \times {10^{ - 13}}{\rm{ }}W \cdot {m^{ - 2}}\).

Step by step solution

01

A concept:

The greater the amplitude, the louder and more intense the sound.

Intensity is the number of incident photons per second per unit area (more precisely, it is energy per unit area per unit time), while frequency refers to the frequency of the photon when referred to as a wave, which is the number of waves in a second.

02

(a) Figure for sound level, intensity, and loudness at given frequencies

First, make a vertical line for a given frequency \(\left( {200{\rm{ }}Hz} \right)\) and draw a horizontal line corresponding to this vertical line then we will get our sound intensity levels in \(dB\) as shown in the figure below.

Threshold of hearing is minimum sound level below which person cann’t hear any sound and loudness for barely audible is \(0\)phons.

From the figure you can see that the horizontal line cross y-axis around \(23{\rm{ }}dB\).

So \(23{\rm{ }}dB\) intensity sound level is barely audible \(t\) is the person.

03

Determine the intensity

Now change this sound intensity level \(\left( {dB} \right)\) \(W \cdot {m^{ - 2}}\) by using the following formula.

\(\beta = 10{\log _{10}}\left( {\frac{I}{{{I_0}}}} \right)\)

Here, \(\beta \) is the sound intensity level in \(dB\), \(I\) is the intensity (in \(W \cdot {m^{ - 2}}\)) of ultrasound wave and \({I_0} = {10^{ - 12}}{\rm{ }}W \cdot {m^{ - 2}}\) is the threshold intensity of hearing.

Sound intensity level is given by,

\(\beta = {\rm{ }}23{\rm{ }}dB\)

Threshold intensity of hearing is,

\({I_0} = {10^{ - 12}}{\rm{ }}W \cdot {m^{ - 2}}\)

Determine the intensity \(l\) for \(\beta = {\rm{ }}23{\rm{ }}dB\) by using following formula.

\(\begin{aligned}{}\frac{\beta }{{10}} = {\log _{10}}\left( {\frac{I}{{{I_0}}}} \right)\\\frac{\beta }{{10}} = {\log _{10}}\left( {\frac{I}{{{I_0}}}} \right)\\\frac{I}{{{I_0}}} = {\left( {10} \right)^{\frac{\beta }{{10}}}}\\I = {I_0}{\left( {10} \right)^{\frac{\beta }{{10}}}}\end{aligned}\)

Now replace \({I_0}\) and \(\beta \) with the given data.

\(\begin{aligned}{}I = {10^{ - 12}}{\left( {10} \right)^{\frac{{23}}{{10}}}}\\ = {10^{ - 12}}{\left( {10} \right)^{2.3}}\\ = 1.3 \times {10^{ - 10}}{\rm{ }}W \cdot {m^{ - 2}}\end{aligned}\)

04

(b) Figure for sound level, intensity, and loudness at given frequencies

First, make a vertical line for a given frequency \(\left( {4000{\rm{ }}Hz} \right)\) and draw a horizontal line corresponding to this vertical line then we will get our sound intensity levels in \(dB\) as shown in the figure

The threshold of hearing is a minimum sound level below which a person can't hear any sound. and loudness for barely audible is \(0\)phons.

From the figure you can see that this horizontal line cross y-axis around \( - 7{\rm{ }}dB\).

So \( - 7{\rm{ }}dB\) intensity sound level is barely audible t is the person.

05

Define the intensity

Now change this sound intensity level \(\left( {dB} \right)\) \(W \cdot {m^{ - 2}}\) by using the following formula.

\(\beta = 10{\log _{10}}\left( {\frac{I}{{{I_0}}}} \right)\)

Here, \(\beta \) is the sound intensity level in \(dB\), \(l\) is the intensity (in \(W \cdot {m^{ - 2}}\)) of ultrasound wave and \({I_0} = {10^{ - 12}}{\rm{ }}W \cdot {m^{ - 2}}\) is the threshold intensity of hearing.

Sound intensity level is,

\(\beta = - 7{\rm{ }}dB\)

Threshold intensity of hearing is,

\({I_0} = {10^{ - 12}}{\rm{ }}W \cdot {m^{ - 2}}\)

Calculate intensity \(I\) for \(\beta = - 7{\rm{ }}dB\) by using following formula.

\(\begin{aligned}{}\frac{\beta }{{10}} = {\log _{10}}\left( {\frac{I}{{{I_0}}}} \right)\\\frac{\beta }{{10}} = {\log _{10}}\left( {\frac{I}{{{I_0}}}} \right)\\\frac{I}{{{I_0}}} = {\left( {10} \right)^{\frac{\beta }{{10}}}}\\I = {I_0}{\left( {10} \right)^{\frac{\beta }{{10}}}}\end{aligned}\)

Now replace \({I_0}\) and \(\beta \) with the given data.

\(\begin{aligned}{}I = {10^{ - 12}}{\left( {10} \right)^{\frac{{ - 7}}{{10}}}}\\ = {10^{ - 12}}{\left( {10} \right)^{ - 0.7}}\\ = 2 \times {10^{ - 13}}{\rm{ }}W \cdot {m^{ - 2}}\end{aligned}\)

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Most popular questions from this chapter

What frequencies will a 1.80 m long tube produce in the audible range at 20.0 C if:

(a) The tube is closed at one end?

(b) It is open at both ends?

(a) Ear trumpets were never very common, but they did aid people with hearing losses by gathering sound over a large area and concentrating it on the smaller area of the eardrum. What decibel increase does an ear trumpet produce if its sound gathering area is\(900\;{\rm{c}}{{\rm{m}}^{\rm{2}}}\)and the area of the eardrum is\(0.500\;{\rm{c}}{{\rm{m}}^{\rm{2}}}\), but the trumpet only has an efficiency of\(5.00\% \)in transmitting the sound to the eardrum? (b) Comment on the usefulness of the decibel increase found in part (a)

Sound is more effectively transmitted into a stethoscope by direct contact than through the air, and it is further intensified by being concentrated on the smaller area of the eardrum. It is reasonable to assume that sound is transmitted into a stethoscope\(100\)times as effectively compared with transmission though the air. What, then, is the gain in decibels produced by a stethoscope that has a sound gathering area of\(15.0\;{\rm{c}}{{\rm{m}}^{\rm{2}}}\), and concentrates the sound onto two eardrums with a total area of\(0.900\;{\rm{c}}{{\rm{m}}^{\rm{2}}}\)with an efficiency of\(40.0\% \)?

Based on the graph inFigure\({\bf{17}}.{\bf{36}}\), what is the threshold of hearing

in decibels for frequencies of\({\bf{60}},{\rm{ }}{\bf{400}},{\rm{ }}{\bf{1000}},{\rm{ }}{\bf{4000}},{\rm{ }}{\bf{and}}{\rm{ }}{\bf{15}},{\bf{000}}{\rm{ }}{\bf{Hz}}\)? Note

that many AC electrical appliances produce 60 Hz, music is commonly

\({\bf{400}}{\rm{ }}{\bf{Hz}}\), a reference frequency is\({\bf{1000}}{\rm{ }}{\bf{Hz}}\), your maximum sensitivity

is near\({\bf{4000}}{\rm{ }}{\bf{Hz}}\), and many older TVs produce a\({\bf{15}},{\bf{750}}{\rm{ }}{\bf{Hz}}\)whine.

You are given two wind instruments of identical length. One is open at both ends, whereas the other is closed at one end. Which is able to produce

the lowest frequency?

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