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Ch 36: Diffraction
Chapter 35, Problem 36

A series of parallel linear water wave fronts are traveling directly toward the shore at 15.0 cm/s on an otherwise placid lake. A long concrete barrier that runs parallel to the shore at a distance of 3.20 m away has a hole in it. You count the wave crests and observe that 75.0 of them pass by each minute, and you also observe that no waves reach the shore at +-61.3 cm from the point directly opposite the hole, but waves do reach the shore everywhere within this distance. (b) At what other angles do you find no waves hitting the shore?

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1
Determine the frequency of the waves by dividing the number of wave crests observed per minute by 60 to convert it to wave crests per second.
Calculate the wavelength of the waves using the formula: wavelength (λ) = wave speed (v) / frequency (f).
Identify the angles at which destructive interference occurs, which corresponds to the minima in the wave pattern. Use the formula for destructive interference in a single-slit diffraction pattern: d \sin(\theta) = (m + 0.5)λ, where d is the width of the slit, \theta is the angle of minima, and m is the order of the minima (m = 0, 1, 2, ...).
Substitute the known values into the formula and solve for \theta for different values of m to find the angles at which no waves hit the shore.
Consider the symmetry of the problem to determine if there are additional angles on both sides of the central maximum (directly opposite the hole) where no waves hit the shore.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Wave Interference

Wave interference occurs when two or more waves overlap and combine to form a new wave pattern. This can result in constructive interference, where wave amplitudes add together, or destructive interference, where they cancel each other out. In the context of the problem, the absence of waves at certain angles indicates destructive interference due to the barrier and the hole, creating regions where wave energy is minimized.
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Diffraction

Diffraction is the bending of waves around obstacles and the spreading of waves when they pass through openings. In this scenario, the waves passing through the hole in the barrier will diffract, creating new wave fronts that spread out. The angles at which no waves reach the shore are determined by the geometry of the hole and the wavelength of the waves, which influences how the waves propagate after passing through the opening.
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Wave Speed and Frequency

The speed of a wave is determined by its frequency and wavelength, described by the equation v = fλ, where v is wave speed, f is frequency, and λ is wavelength. In this problem, the wave speed is given as 15.0 cm/s, and the frequency can be calculated from the number of wave crests observed per minute. Understanding the relationship between speed, frequency, and wavelength is crucial for analyzing how waves interact with barriers and openings.
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Related Practice
Textbook Question
Light of wavelength 585 nm falls on a slit 0.0666 mm wide. (a) On a very large and distant screen, how many totally dark fringes (indicating complete cancellation) will there be, including both sides of the central bright spot? Solve this problem without calculating all the angles! (Hint: What is the largest that sin u can be? What does this tell you is the largest that m can be?) (b) At what angle will the dark fringe that is most distant from the central bright fringe occur?
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Textbook Question
Diffraction occurs for all types of waves, including sound waves. High-frequency sound from a distant source with wavelength 9.00 cm passes through a slit 12.0 cm wide. A microphone is placed 8.00 m directly in front of the center of the slit, corresponding to point O in Fig. 36.5a . The microphone is then moved in a direction perpendicular to the line from the center of the slit to point O. At what distances from O will the intensity detected by the microphone be zero?
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Textbook Question
A series of parallel linear water wave fronts are traveling directly toward the shore at 15.0 cm/s on an otherwise placid lake. A long concrete barrier that runs parallel to the shore at a distance of 3.20 m away has a hole in it. You count the wave crests and observe that 75.0 of them pass by each minute, and you also observe that no waves reach the shore at +-61.3 cm from the point directly opposite the hole, but waves do reach the shore everywhere within this distance. (a) How wide is the hole in the barrier?
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Textbook Question
Monochromatic light of wavelength 580 nm passes through a single slit and the diffraction pattern is observed on a screen. Both the source and screen are far enough from the slit for Fraunhofer diffraction to apply. (a) If the first diffraction minima are at +-90.0°, so the central maximum completely fills the screen, what is the width of the slit? (b) For the width of the slit as calculated in part (a), what is the ratio of the intensity at u = 45.0° to the intensity at u = 0?
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Textbook Question
A slit 0.240 mm wide is illuminated by parallel light rays of wavelength 540 nm. The diffraction pattern is observed on a screen that is 3.00 m from the slit. The intensity at the center of the central maximum (u = 0°) is 6.00 x 10^-6 W/m2. (a) What is the distance on the screen from the center of the central maximum to the first minimum?
294
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Textbook Question
A slit 0.240 mm wide is illuminated by parallel light rays of wavelength 540 nm. The diffraction pattern is observed on a screen that is 3.00 m from the slit. The intensity at the center of the central maximum (u = 0°) is 6.00 x 10^-6 W/m2. (b) What is the intensity at a point on the screen midway between the center of the central maximum and the first minimum?
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