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At a distance of \(20.0 \mathrm{~m}\) from a sound source, the intensity of the sound is \(60.0 \mathrm{~dB}\). What is the intensity (in \(\mathrm{dB}\) ) at a point \(2.00 \mathrm{~m}\) from the source? Assume that the sound radiates equally in all directions from the source.

Short Answer

Expert verified
Answer: The intensity at a point 2.00 m from the source is 100 dB.

Step by step solution

01

Define the inverse square law for intensity with respect to distance

The inverse square law dictates that the ratio of the intensities is proportional to the inverse square of the ratio of the distances. We can define this mathematically as follows: \(I_1 / I_2 = (d_2 / d_1)^2\)
02

Convert decibels to intensity

Given the intensity in decibels, we need to convert it to Watts per square meter (W/m²). The formula for converting decibels to intensity is: \(I = 10^{L/10} \times 10^{-12} \mathrm{~W/m²}\) First, use the provided intensity level \(60.0 \mathrm{~dB}\) and convert it to intensity (W/m²): \(I_1 = 10^{60/10} \times 10^{-12} = 10^6 \times 10^{-12} = 10^{-6} \mathrm{~W/m²}\)
03

Use the inverse square law formula to find the new intensity

Now that we have the initial intensity \(I_1\) and the distances \(d_1 = 20.0 \mathrm{~m}\) and \(d_2 = 2.00 \mathrm{~m}\), we can plug in the values to the inverse square law formula: \(I_2 = I_1 \times (d_1 / d_2)^2 = 10^{-6} \mathrm{~W/m²} \times (20.0 \mathrm{~m} / 2.00 \mathrm{~m})^2\)
04

Solve for the new intensity

From the previous step, we get: \(I_2 = 10^{-6} \mathrm{~W/m²} \times (10)^2 = 10^{-6} \mathrm{~W/m²} \times 100 = 10^{-4} \mathrm{~W/m²}\)
05

Convert back to decibels

Now, we need to convert the new intensity (in W/m²) back to decibels. The formula for converting intensity to decibels is: \(L = 10 \log_{10}(I / 10^{-12})\) Plug in the calculated intensity and find the new intensity level: \(L_2 = 10 \log_{10}(10^{-4} \mathrm{~W/m²} / 10^{-12}) = 100 \mathrm{~dB}\) The intensity at a point 2.00 m from the source is \(100 \mathrm{~dB}\).

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Key Concepts

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

Understanding the Inverse Square Law
The inverse square law is a physical principle that describes how certain quantities decrease in strength as they spread out from a source. When it comes to sound intensity, this law tells us that as you move away from a sound source, the intensity of the sound diminishes rapidly. Specifically, the intensity is inversely proportional to the square of the distance from the source. To put it in simpler terms, if you double the distance from the source, the sound intensity becomes one-fourth of its original value.

This relationship is crucial for understanding how sound behaves in a three-dimensional space. In the context of the exercise, by using the inverse square law, we can calculate how much quieter a sound will be at a certain distance compared to another point. The formula expressed mathematically is \(I_1 / I_2 = (d_2 / d_1)^2\), where \(I_1\) and \(I_2\) are the sound intensities at two different distances, \(d_1\) and \(d_2\), from the sound source.
Intensity Conversion Between Decibels and Watts per Square Meter
Sound intensity can be measured in two different units: decibels (dB), which is a logarithmic unit, and watts per square meter (W/m²), a linear unit. Converting between these units is a common step in solving problems related to sound intensity.

To convert from decibels to watts per square meter, we use the formula \(I = 10^{L/10} \times 10^{-12} \mathrm{~W/m^2}\), where \(L\) is the sound intensity level in decibels. Conversely, to convert from watts per square meter to decibels, you would use \(L = 10 \log_{10}(I / 10^{-12})\). These formulas account for the fact that the decibel scale is logarithmic, meaning each step on the scale represents a factor of change, and the applicable baseline intensity for decibels in acoustics is typically \(10^{-12} \mathrm{~W/m^2}\), which corresponds to the threshold of human hearing.

Using these formulas, students can easily switch between a linear representation of sound intensity (which makes calculating changes over distance straightforward) and the more commonly used decibel scale.
The Logarithmic Scale of Decibels
The concept of a logarithmic scale is essential when discussing sound intensity levels measured in decibels. A logarithmic scale is used to represent a wide range of values in a more compact and manageable way. In the case of sound, the range of human hearing spans from the quietest sound at 0 dB (the threshold of hearing) to sounds that are damagingly loud, which can be over 120 dB. A logarithmic scale is helpful here because it allows us to handle these large variations with smaller, more intuitive numbers.

The decibel system is a relative scale that compares the measured intensity to a reference value. It's based on powers of 10, following the formula \(L = 10 \log_{10}(I / I_0)\), where \(L\) is the sound level in decibels, \(I\) is the sound intensity, and \(I_0\) is the reference intensity. Every 10 dB increase represents a tenfold increase in the sound intensity, and every 20 dB increase represents a hundredfold increase. This is why in our exercise, a relatively small change in distance results in a large change in decibel level—because the decibel scale compresses changes exponentially.

Appreciating the logarithmic nature of the decibel scale helps students understand why distances impact sound intensity levels so dramatically and why such calculations are fundamental in fields concerned with noise management and audio engineering.

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Most popular questions from this chapter

Compare the intensity of sound at the pain level, \(120 \mathrm{~dB}\), with that at the whisper level, \(20 \mathrm{~dB}\).

A police siren contains at least two frequencies, producing the wavering sound (beats). Explain how the siren sound changes as a police car approaches, passes, and moves away from a pedestrian.

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.

When two pure tones with similar frequencies combine to produce beats, the result is a train of wave packets. That is, the sinusoidal waves are partially localized into packets. Suppose two sinusoidal waves of equal amplitude A, traveling in the same direction, have wave numbers \(\kappa\) and \(\kappa+\Delta \kappa\) and angular frequencies \(\omega\) and \(\omega+\Delta \omega\), respectively. Let \(\Delta x\) be the length of a wave packet, that is, the distance between two nodes of the envelope of the combined sine functions. What is the value of the product \(\Delta x \Delta \kappa ?\)

A college student is at a concert and really wants to hear the music, so she sits between two in-phase loudspeakers, which point toward each other and are \(50.0 \mathrm{~m}\) apart. The speakers emit sound at a frequency of \(490 .\) Hz. At the midpoint between the speakers, there will be constructive interference, and the music will be at its loudest. At what distance closest to the midpoint could she also sit to experience the loudest sound?

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