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Two loudspeakers, \(4.0 \mathrm{m}\) apart and facing each other, play identical sounds of the same frequency. You stand halfway between them, where there is a maximum of sound intensity. Moving from this point toward one of the speakers, you encounter a minimum of sound intensity when you have moved \(0.25 \mathrm{m}\). a. What is the frequency of the sound? b. If the frequency is then increased while you remain \(0.25 \mathrm{m}\) from the center, what is the first frequency for which that location will be a maximum of sound intensity?

Short Answer

Expert verified
a) The frequency of the sound is \(686 \mathrm{Hz}\). b) The first frequency for which that location will be a maximum of sound intensity is \(1372 \mathrm{Hz}\).

Step by step solution

01

Identify the relevant equations

The speed of sound in air is typically around \(343 \mathrm{m/s}\). The phase difference between waves from two points is given by \(2\pi/\lambda \times \text{path difference}\), and in case of destructive interference it should equal to \(\pi\), an odd multiple of \(\pi\). And, the frequency of the wave is determined by the formula \(v = f\lambda\), where \(v\) is the velocity of the sound, \(f\) is the frequency and \(\lambda\) is the wavelength.
02

Solve for the frequency

Given a path difference of \(0.25\mathrm{m}\) leads to a first minimum of sound intensity, it inferes that the wavelength \(\lambda\) of the sound wave will be \(2 \times 0.25\mathrm{m} = 0.50\mathrm{m}\). Substituting the values into the formula for frequency, we get \(f = v/\lambda =343 \mathrm{m/s} /0.5 \mathrm{m} = 686 \mathrm{Hz}\).
03

Find the next increase in frequency causing a maximum

For maximal sound intensity, the phase difference should equal to \(2\pi\), a multiple of \(2\pi\). So the wavelength for the next maximum will be simply equal to the path difference, i.e., \(0.25 \mathrm{m}\). Substituting the values into the formula for frequency, we get \(f = v/\lambda =343 \mathrm{m/s} /0.25 \mathrm{m} = 1372 \mathrm{Hz}\).

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Key Concepts

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

Frequency Calculation
Let's start with understanding how frequency calculation plays a role in sound interference. Frequency tells us how many oscillations per second a sound wave makes. It's crucial because it determines the pitch of the sound. In this scenario, you're dealing with sound waves coming from two loudspeakers. To find the frequency, you need to use the formula:\[ v = f \lambda \]where \( v \) is the speed of sound, \( f \) is the frequency, and \( \lambda \) is the wavelength. Given that the speed of sound is approximately \(343\ \text{m/s}\), and the wavelength was deduced to be \(0.5\ \text{m}\), you can calculate the frequency as follows:\[ f = \frac{v}{\lambda} = \frac{343\ \text{m/s}}{0.5\ \text{m}} = 686\ \text{Hz} \]This result, \(686\ \text{Hz}\), is the frequency where you initially observe a minimum in sound intensity.
It's essential to remember this frequency, as it will help in further steps when determining conditions for maximum sound intensity.
Sound Intensity
Sound intensity is essential in understanding sound wave interference. It measures how much sound energy passes through a certain area. Imagine standing equidistant between two loudspeakers. Here, sound waves interfere with each other, creating areas of high and low intensity.
When sound waves constructively interfere—they enhance each other's effect, creating a "maximum" of sound intensity. Conversely, destructive interference leads to a "minimum" of sound intensity, where waves cancel each other out.
  • At a maximum, the waves are in phase.
  • At a minimum, they are out of phase.
In this exercise, you first noted a minimum intensity at a displacement of \(0.25\ \text{m}\) from the midway point—an indicator of destructive interference. By changing the sound frequency, you influence where these maxima and minima occur.
This exercise demonstrates the positions along the line between the speakers where constructive or destructive interference will cause peaks or nulls in sound intensity.
Wavelength Determination
Understanding how wavelength is determined is key in sound wave problems. The wavelength \( \lambda \) is the distance between successive peaks of a wave. It's related to the wave's speed and frequency by the equation \( v = f \lambda \). For sound waves in air, the speed \( v \) is approximately \(343\ \text{m/s}\). In this exercise, when you first notice a minimum of sound intensity at \(0.25\ \text{m}\) from the center, it gives you a clue about the wavelength of the sound.- At a minimum of intensity, the path difference is half of the wavelength.
- Thus, the wavelength \( \lambda \) can be calculated as: \[ \lambda = 2 \times \text{path difference} = 2 \times 0.25\ \text{m} = 0.5\ \text{m} \]Why is calculating wavelength important? Knowing \( \lambda \) not only allows us to find frequency but also helps determine the spatial distribution of interference patterns.
When the frequency changes, affecting \( \lambda \), the pattern of sound intensity shifts, affecting where maxima and minima will occur. With a new maximum, you discover the location's conditions for optimal sound experience.

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Most popular questions from this chapter

Piano tuners tune pianos by listening to the beats between the harmonics of two different strings. When properly tuned, the note A should have the frequency \(440 \mathrm{Hz}\) and the note E should be at \(659 \mathrm{Hz}\). The tuner can determine this by listening to the beats between the third harmonic of the A and the second harmonic of the E. A tuner first tunes the A string very precisely by matching it to a \(440 \mathrm{Hz}\) tuning fork. She then strikes the A and \(\mathrm{E}\) strings simultaneously and listens for beats between the harmonics. What beat frequency indicates that the E string is properly tuned?

When a sound wave travels directly toward a hard wall, the incoming and reflected waves can combine to produce a standing wave. There is an antinode right at the wall, just as at the end of a closed tube, so the sound near the wall is loud. You are standing beside a brick wall listening to a \(50 \mathrm{Hz}\) tone from a distant loudspeaker. How far from the wall must you move to find the first quiet spot? Assume a sound speed of \(340 \mathrm{m} / \mathrm{s}\).

When you voice the vowel sound in "hat," you narrow the opening where your throat opens into the cavity of your mouth so that your vocal tract appears as two connected tubes. The first is in your throat, closed at the vocal cords and open at the back of the mouth. The second is the mouth itself, open at the lips and closed at the back of the mouth-a different condition than for the throat because of the relatively larger size of the cavity. The corresponding formant frequencies are \(800 \mathrm{Hz}\) (for the throat) and \(1500 \mathrm{Hz}\) (for the mouth). What are the lengths of these two cavities? Assume a sound speed of \(350 \mathrm{m} / \mathrm{s}\).

A particularly beautiful note reaching your ear from a rare Stradivarius violin has a wavelength of \(39.1 \mathrm{cm} .\) The room is slightly warm, so the speed of sound is \(344 \mathrm{m} / \mathrm{s}\). If the string's linear density is \(0.600 \mathrm{g} / \mathrm{m}\) and the tension is \(150 \mathrm{N},\) how long is the vibrating section of the violin string?

In addition to producing images, ultrasound can be used to heat tissues of the body for therapeutic purposes. An emitter is placed against the surface of the skin; the amplitude of the ultrasound wave at this point is quite large. When a sound wave hits the boundary between soft tissue and bone, most of the energy is reflected. The boundary acts like the closed end of a tube, which can lead to standing waves. Suppose \(0.70 \mathrm{MHz}\) ultrasound is directed through a layer of tissue with a bone \(0.55 \mathrm{cm}\) below the surface. Will standing waves be created? Explain.

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