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Two loudspeakers, \(A\) and \(B\), are driven by the same amplifier and emit sinusoidal waves in phase. Speaker \(B\) is \(12.0 \mathrm{~m}\) to the right of speaker \(A\). The frequency of the waves emitted by each speaker is \(688 \mathrm{~Hz}\). You are standing between the speakers, along the line connecting them, and are at a point of constructive interference. How far must you walk toward speaker \(B\) to move to a point of destructive interference?

Short Answer

Expert verified
To reach a point of destructive interference from a point of constructive interference, one must travel a distance equal to half the wavelength.

Step by step solution

01

Calculate the wavelength of the sound wave

Utilize the relationship between the speed of sound (\(v\)), frequency (\(f\)), and wavelength (\(\lambda\)). This relation is expressed as \(v = f \times \lambda\). Rearranging the equation to isolate \(\lambda\), we have \(\lambda = v / f\). Here, the speed of sound in air (\(v\)) is approximately \(343 m/s\) (under normal conditions) and the frequency (\(f\)) is given as \(688 Hz\).
02

Determine the distance between constructive and destructive interference points

The distance between two points of destructive interference or two points of constructive interference is one wavelength (\(\lambda\)). However, moving from a point of constructive interference to the next point of destructive interference requires to travel half a wavelength, or \(\lambda / 2\).
03

Calculate the distance to travel to reach a point of destructive interference from a point of constructive interference

This distance is half the wavelength minus the initial distance from speaker A. However, since the observers stand midway between the speakers, the distance is simply half the wavelength, or \(\lambda / 2\).

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Key Concepts

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

Understanding Constructive Interference
When two sound waves meet and are in phase, they can combine and create a wave with a greater amplitude. This is known as constructive interference. Think of it like pushing someone on a swing at just the right moment. If you push as they move forward, they go even higher. The principle of constructive interference is based on the alignment of wave crests and troughs from different sources.

In the example of speakers A and B, each emits a wave with the same frequency and is in phase. This setup allows their sound waves to align and amplify wherever they meet. It's like both speakers are singing a harmony that combines into a louder sound at certain points. If you are at such a point, you are experiencing constructive interference due to the consistent lines of the wave peaks meeting each other.

To determine where these points are, we rely on the wavelength of the sound. These points occur at regular intervals all along the path between the two speakers.
  • Constructive interference happens when waves reinforce each other.
  • Occurs at intervals of full wavelengths from a speaker.
  • Results in a louder sound.
Exploring Destructive Interference
Destructive interference occurs when two waves meet and are out of phase. Imagine you are trying to push someone on a swing just as they are coming toward you—you push them backward instead of lifting them higher. When two sound waves are out of sync, one wave's crest aligns with another wave's trough, effectively canceling each other out and reducing the sound's amplitude.

In a scenario with two speakers, standing at a point of destructive interference means that the sound waves from both speakers are cancelling each other as they meet at that spot. This effect produces a much quieter area or even a spot of silence in some cases. Moving from a point where the sound is loud due to constructive interference to a quieter spot involves shifting by half the wavelength of the sound wave being emitted by the speakers.

To transition from constructive to destructive:
  • Move half a wavelength distance (\(\frac{\lambda}{2}\)
  • Wave crests from one source align with troughs from another.
  • Results in much quieter or silent zones.
Nature of Sound Waves
Sound waves are vibrations that travel through the air and can be heard when they reach a person's or animal's ear. These waves are created when an object (such as a speaker diaphragm) vibrates, causing the nearby molecules to compress and then spread out in a pattern.

Understanding a few key properties helps grasp how sound behaves:- **Frequency**: This describes how many cycles a wave completes in a second, measured in Hertz (Hz). Human hearing typically ranges between 20 Hz to 20,000 Hz.- **Wavelength**: The distance between successive crests, troughs, or identical points of the wave. Related to speed and frequency by the formula \(\lambda = v / f\), where \(\lambda\) is the wavelength, \(v\) is the speed (343 m/s in air), and \(f\) is frequency.- **Amplitude**: Related to how "loud" a sound is. Greater amplitudes mean higher energy and therefore louder sounds.

Sound waves can interfere with each other constructively or destructively based on how these properties align. This interference principle helps define how we experience sound in different environments, such as the exercise scenario with two speakers and an observer.
  • Sound waves are pressure waves traveling through mediums.
  • Consist of properties like frequency, wavelength, and amplitude.
  • Interference patterns affect how we perceive sound loudness.

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Most popular questions from this chapter

On the planet Arrakis a male ornithoid is flying toward his mate at \(25.0 \mathrm{~m} / \mathrm{s}\) while singing at a frequency of \(1200 \mathrm{~Hz}\). If the stationary female hears a tone of \(1240 \mathrm{~Hz}\), what is the speed of sound in the atmosphere of Arrakis?

The shock-wave cone created by a 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 \(344 \mathrm{~m} / \mathrm{s} ?\)

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?

Many professional singers have a range of \(2 \frac{1}{2}\) octaves or even greater. Suppose a soprano's range extends from A below middle C (frequency \(220 \mathrm{~Hz}\) ) up to E-flat above high \(\mathrm{C}\) (frequency \(1244 \mathrm{~Hz}\) ). Although the vocal tract is complicated, we can model it as a resonating air column, like an organ pipe, that is open at the top and closed at the bottom. The column extends from the mouth down to the diaphragm in the chest cavity. Assume that the lowest note is the fundamental. How long is this column of air if \(v=354 \mathrm{~m} / \mathrm{s} ?\) Does your result seem reasonable, on the basis of observations of your body?

You blow across the open mouth of an empty test tube and produce the fundamental standing wave in the \(14.0-\mathrm{cm}\) -long air column in the test tube, which acts as a stopped pipe. (a) What is the frequency of this standing wave? (b) What is the frequency of the fundamental standing wave in the air column if the test tube is half filled with water?

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