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Two sources as in phase and emit waves with \(\lambda=0.42 \mathrm{m}\). Determine whether constructive or destructive interference occurs at points whose distances from the two sources are (a) 0.84 and \(0.42 \mathrm{m}\), (b) 0.21 and \(0.42 \mathrm{m},\) (c) 1.26 and \(0.42 \mathrm{m},\) (d) 1.87 and \(1.45 \mathrm{m},\) (e) 0.63 and \(0.84 \mathrm{m}\) and \((\mathrm{f}) 1.47\) and \(1.26 \mathrm{m}\).

Short Answer

Expert verified
(a) Constructive interference (b) Destructive interference (c) Constructive interference (d) Constructive interference (e) Destructive interference (f) Destructive interference

Step by step solution

01

Identify the constructive and destructive interference conditions

For constructive interference, the path difference between the two sources should be an integer multiple of the wavelength (nλ). For destructive interference, the path difference must be an odd multiple of half the wavelength (nλ + λ/2). Constructive interference: \(PathDifference = n\lambda\) Destructive interference: \(PathDifference = n\lambda + \frac{\lambda}{2}\), where n is an integer (including 0), and λ is the wavelength.
02

Calculate the path difference for each point

For each given point, calculate the path difference by finding the absolute difference between the distances from the two sources. (a) \(|0.84 - 0.42| = 0.42 \mathrm{m}\) (b) \(|0.21 - 0.42| = 0.21 \mathrm{m}\) (c) \(|1.26 - 0.42| = 0.84 \mathrm{m}\) (d) \(|1.87 - 1.45| = 0.42 \mathrm{m}\) (e) \(|0.63 - 0.84| = 0.21 \mathrm{m}\) (f) \(|1.47 - 1.26| = 0.21 \mathrm{m}\)
03

Assess constructive or destructive interference for each point

For each path difference, check whether the value matches an integer multiple of the wavelength (constructive interference) or an odd multiple of half the wavelength (destructive interference). (a) \(0.42 \mathrm{m}\): Constructive interference, as \(0.42 = 1\cdot(0.42)\) (b) \(0.21 \mathrm{m}\): Destructive interference, as \(0.21 = 1\cdot(0.42/2)\) (c) \(0.84 \mathrm{m}\): Constructive interference, as \(0.84 = 2\cdot(0.42)\) (d) \(0.42 \mathrm{m}\): Constructive interference, as \(0.42 = 1\cdot(0.42)\) (e) \(0.21 \mathrm{m}\): Destructive interference, as \(0.21 = 1\cdot(0.42/2)\) (f) \(0.21 \mathrm{m}\): Destructive interference, as \(0.21 = 1\cdot(0.42/2)\)
04

Summarize the results

To summarize, we have the following types of interference occurring at each point: (a) Constructive interference (b) Destructive interference (c) Constructive interference (d) Constructive interference (e) Destructive interference (f) Destructive interference

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Key Concepts

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

Constructive Interference
When the waves from two sources meet and their effects add together, you have constructive interference. This happens when the peaks or troughs of both waves align perfectly, creating a wave with greater amplitude. For this to occur, the path difference between the waves must be an integer multiple of the wavelength.
If each wave is like a series of hills (peaks) and valleys (troughs), constructive interference means the hills and hills meet, and the valleys and valleys meet, stacking on top of each other.
Thus, if the path difference is given by \( n\lambda \) where \( n \) is an integer, this is constructive interference. It makes the sound louder, the light brighter, or the surface more disturbed if waves are in water. In our exercise, points where the path difference is a direct multiple of the wavelength, such as 0.42 m and 0.84 m, exhibit constructive interference.
Destructive Interference
Destructive interference is the opposite of constructive interference. Here, when the waves meet, they cancel each other out. Instead of creating a bigger wave, they diminish or nullify the wave effect.
This occurs when one wave's peak aligns with the other's valley. The mathematical condition for destructive interference is a path difference of an odd multiple of half the wavelength.
Essentially, if the path difference is given by \( n\lambda + \frac{\lambda}{2} \), where \( n \) is an integer, the waves will interfere destructively.
In practice, this might mean quieter sound or dimmer light. In this exercise, the path differences of 0.21 m produce destructive interference, as these are odd multiples of half the wavelength 0.42 m.
Path Difference
In wave interference, path difference is crucial in determining the type of interference you'll observe. It's simply the absolute difference between the distances covered by two waves from their respective sources to a specific point.
Imagine you and a friend are walking from separate points to meet at a bench. The path difference is like checking whose route took longer in distance terms.
For example, if one wave travels 0.84 m and another 0.42 m but are from the same source, the path difference is \(|0.84 - 0.42| = 0.42 \mathrm{m}\). This value determines whether the interference is constructive (if a whole number times the wavelength) or destructive (if an odd half-multiple of the wavelength). Understanding and calculating path difference is essential for predicting interference patterns.
Phase
In physics, phase refers to the position of a point in time on a waveform cycle. Two waves that start together are in-phase, meaning they reach similar points on their wave cycles simultaneously.
When waves are in-phase, and their path difference satisfies constructive interference conditions, it contributes to a bigger and stronger resultant wave, enhancing phenomena such as light brightness or sound volume.
Conversely, if they are out of phase by half a wavelength, they can destructively interfere, leading to nullification.
The phase relation determines if waves will amplify or nullify each other, contributing significantly to the practical uses of wave interference, such as noise-canceling technology.
Wavelength Calculation
The wavelength is a measure of the distance between sequential peaks or troughs in a wave. It is a fundamental property defining how waves propagate through space.
Wavelength, denoted as \( \lambda \), is generally calculated by measuring the distance over which the wave's shape repeats. In many exercises, understanding and being able to calculate the wavelength helps to solve for interference types.
In our exercise, a given wavelength of 0.42 m helps to determine which interferences are constructive or destructive by comparing path differences against it.
For students, mastering wavelength calculation involves practicing problems where they identify the spacing between peaks or troughs to accurately determine the type and result of wave interactions.

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Most popular questions from this chapter

In placing a sample on a microscope slide, a glass cover is placed over a water drop on the glass slide. Light incident from above can reflect from the top and bottom of the glass cover and from the glass slide below the water drop. At which surfaces will there be a phase change in the reflected light?

A Michelson interferometer with a He-Ne laser light source \((\lambda=632.8 \mathrm{nm})\) projects its interference pattern on a screen. If the movable mirror is caused to move by \(8.54 \mu \mathrm{m},\) how many fringes will be observed shifting through a reference point on a screen?

What effect does increasing the wedge angle have on the spacing of interference fringes? If the wedge angle is too large, fringes are not observed. Why?

A hydrogen gas discharge lamp emits visible light at four wavelengths, \(\lambda=410,434,486,\) and \(656 \mathrm{nm}\) (a) If light from this lamp falls on a \(N\) slits separated by \(0.025 \mathrm{mm},\) how far from the central maximum are the third maxima when viewed on a screen \(2.0 \mathrm{m}\) from the slits? (b) By what distance are the second and third maxima separated for \(l=486 \mathrm{nm}\) ?

A film of oil on water will appear dark when it is very thin, because the path length difference becomes small compared with the wavelength of light and there is a phase shift at the top surface. If it becomes dark when the path length difference is less than one-fourth the wavelength, what is the thickest the oil can be and appear dark at all visible wavelengths? Oil has an index of refraction of \(1.40 .\)

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