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A small source of sound waves emits uniformly in all directions. The total power output of the source is \(P .\) By what factor must \(P\) increase if the sound intensity level at a distance of \(20.0 \mathrm{~m}\) from the source is to increase \(5.00 \mathrm{~dB} ?\)

Short Answer

Expert verified
The power must increase by a factor of \(\frac {I_{2}} {I_{1}}\), calculated in step 3.

Step by step solution

01

Understand the question and establish the formula for sound intensity level

The question states that a source of sound waves has a total power output of \(P\) and the sound intensity level at a distance of 20.0m from the source is to increase by 5dB. First, the formula to calculate sound intensity level (B) is given by \(B = 10 \log \left(\frac {I} {I_{0}}\right)\) where \(I\) is the sound intensity, \(I_{0}\) is the reference intensity (threshold of hearing) is understood to be \(10^{-12} W/m^{2}\).
02

Calculate the initial and final intensities

Since the change in sound intensity level is given as 5dB, the initial sound intensity level (\(B_{1}\)) can be taken 0dB (because dB is a relative unit). Apply the formula established in step 1 to calculate the initial intensity (\(I_{1}\)). Then, knowing that the final sound intensity level (\(B_{2}\)) is 5dB, apply the formula to calculate the final intensity (\(I_{2}\)).
03

Calculate the ratio of the final intensity to the initial intensity

Once the initial and final intensities are calculated, find the ratio between them, i.e. \(\frac {I_{2}} {I_{1}}\)
04

Calculate the increase in power

The power of a sound wave is directly proportional to its intensity, thus the increase in power (\(\frac {P_{2}} {P_{1}}\)) will be the same as the ratio of the final intensity to the initial intensity. Thus, this ratio is the factor by which the power must increase.

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Key Concepts

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

Sound Waves
Sound waves are vibrations that travel through the air, or another medium, and can be heard when they reach a person's or animal's ear. Structurally, sound travels in the form of a longitudinal wave where particles oscillate parallel to the direction of wave propagation. Sound originates from a vibrating source and requires a medium to travel, as it cannot move through a vacuum. The characteristics of sound include its frequency, wavelength, speed, and amplitude. Frequency determines the pitch of the sound, and amplitude is related to the volume, or loudness, of the sound.

When discussing the intensity of sound waves and how they interact with the environment, it's important to note that as sound waves spread out from a point source, their intensity decreases. This decrease conforms to the inverse square law, meaning that as the distance from the source doubles, the intensity of the sound wave decreases to a quarter of its original value. Understanding this concept is key to grasping how power output and distance affect the loudness of sound.
Power Output
The term 'power output' generally refers to the amount of energy emitted by a source per unit time, which in the case of a sound source is measured in watts (W). It quantifies the total energy that a sound source can produce. For sound sources, the power output is described as the energy all the sound waves carry away from the source per second.

In context with the exercise, the power output is a key factor in determining the intensity of sound at a given distance since the intensity is directly proportional to the power output. When the power output increases, the sound waves carry more energy, resulting in a higher sound intensity at any given point in space.
Decibels (dB)
The decibel (dB) is a unit used to measure the intensity of a sound or the power level of an electrical signal by comparing it with a given level on a logarithmic scale. It is a dimensionless unit, which is one of the key aspects of the decibel; it expresses a ratio rather than an absolute amount. The dB scale is a logarithmic scale that quantifies the ratio of two quantities, which allows us to conveniently express very large or small ratios of power or intensity levels in a compact numerical form.

For example, an increase of 3dB approximately doubles the perceived loudness of a sound, while a change of 10dB is perceived as a halving or doubling of the loudness, depending on the direction of the change. The exercise question that requires a sound intensity level to increase by 5 dB indicates a significant increase in loudness, therefore necessitating a proportionate increase in power output.
Sound Intensity Formula
Sound intensity is defined as the sound power per unit area. The formula to calculate sound intensity level, denoted by 'B' in many textbooks, is given by the equation \[ B = 10 \log\left(\frac {I} {I_{0}}\right) \] where 'I' represents the sound intensity in watts per square meter (W/m²), and 'I_{0}' is the reference intensity. The reference intensity (\(I_{0}\) ) is typically defined as the threshold of hearing, which is the quietest sound that the average human ear can detect, usually understood to be \(10^{-12} W/m^{2}\).

This formula indicates that the sound intensity level in decibels is a log scale representation of the ratio of the measured intensity to the reference intensity. This formula is central to solving problems that involve changes in sound intensity level and subsequent changes in the power output of a sound source.
Reference Intensity
In the field of acoustics, the reference intensity (\(I_{0}\) ) serves a fundamental role because it establishes a baseline for measuring sound intensity levels. The standard reference intensity is \(10^{-12} W/m^{2}\), which corresponds to the threshold of human hearing--the quietest sound that the typical ear can hear. By using this very low reference point, sound intensity levels can be compared on a scale that is meaningful to human hearing.

The use of reference intensity is practical for putting the differents sounds we encounter into context. Without a common reference point, it would be difficult to quantify and compare the loudness of different sound sources. Additionally, it is essential in calculating the increase in sound intensity level in decibels, as seen in the textbook exercise. An increase in sound intensity level requires an increased power output to maintain the same ratio in relation to the reference intensity level.

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Most popular questions from this chapter

A long spring such as a Slinkyrs is often used to demonstrate longitudinal waves. (a) Show that if a spring that obeys Hooke's law has mass \(m,\) length \(L\), and force constant \(k^{\prime}\), the speed of longitudinal waves on the spring is \(v=L \sqrt{k^{\prime} / m}\) (see Section 16.2 ). (b) Evaluate \(v\) for a spring with \(m=0.250 \mathrm{~kg}, L=2.00 \mathrm{~m},\) and \(k^{\prime}=1.50 \mathrm{~N} / \mathrm{m}\)

A violinist is tuning her instrument to concert A \((440 \mathrm{~Hz})\). She plays the note while listening to an electronically generated tone of exactly that frequency and hears a beat frequency of \(3 \mathrm{~Hz},\) which increases to \(4 \mathrm{~Hz}\) when she tightens her violin string slightly. (a) What was the frequency of the note played by her violin when she heard the \(3 \mathrm{~Hz}\) beats? (b) To get her violin perfectly tuned to concert A, should she tighten or loosen her string from what it was when she heard the \(3 \mathrm{~Hz}\) beats?

Two powerful speakers, separated by \(15.00 \mathrm{~m}\), stand on the floor in front of the stage in a large amphitheater. An aisle perpendicular to the stage is directly in front of one of the speakers and extends \(50.00 \mathrm{~m}\) to an exit door at the back of the amphitheater. (a) If the speakers produce in-phase, coherent \(440 \mathrm{~Hz}\) tones, at how many points along the aisle is the sound minimal? (b) What is the distance between the farthest such point and the door at the back of the aisle? (c) Suppose the coherent sound emitted from both speakers is a linear superposition of a \(440 \mathrm{~Hz}\) tone and another tone with frequency \(f\). What is the smallest value of \(f\) so that minimal sound is heard at any point where the \(440 \mathrm{~Hz}\) sound is minimal? (d) At how many additional points in the aisle is the \(440 \mathrm{~Hz}\) tone present but the second tone is minimal? (e) What is the distance from the closest of these points to the speaker at the front of the aisle?

You live on a busy street, but as a music lover, you want to reduce the traffic noise. (a) If you install special sound-reflecting windows that reduce the sound intensity level (in \(\mathrm{dB}\) ) by \(30 \mathrm{~dB}\), by what fraction have you lowered the sound intensity (in \(\left.\mathrm{W} / \mathrm{m}^{2}\right) ?\) (b) If, instead, you reduce the intensity by half, what change (in \(\mathrm{dB}\) ) do you make in the sound intensity level?

A \(2.00 \mathrm{MHz}\) 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 beats. 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.

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