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In a two-slit interference pattern, the intensity at the peak of the central maximum is \(I_{0}\). (a) At a point in the pattern where the phase difference between the waves from the two slits is \(60.0^{\circ}\), what is the intensity? (b) What is the path difference for \(480 \mathrm{nm}\) light from the two slits at a point where the phase difference is \(60.0^{\circ} ?\)

Short Answer

Expert verified
The intensity at a point in the pattern where the phase difference between the waves from the two slits is \(60.0^{\circ}\) is equal to \(I_0 / 4\). The path difference for \(480 \mathrm{nm}\) light from the two slits at a point where the phase difference is \(60.0^{\circ}\) is \(80 \mathrm{nm}\).

Step by step solution

01

Calculate the Intensity

The formula to calculate the intensity in an interference pattern is given by \(I = I_{0} \cos^{2}(\phi / 2)\). Here, \(\phi\) denotes the phase difference and \(I_{0}\) represents the peak intensity. We are given that \(\phi = 60.0^{\circ}\) and \(I_{0}\) is the intensity at the peak of the central maximum. Convert the phase difference to radians, as the trigonometric function in the formula works with radian measures. After conversion, \(\phi = \pi / 3\). Now, substitute the values into the equation to find the intensity.
02

Compute Path Difference

The path difference can be computed using the formula \(d = \lambda \phi / (2\pi)\), Where \(d\) represents the path difference, \(\lambda\) denotes the wavelength of the light, and \(\phi\) is the phase difference. Substituting the given values, \(\phi = \pi / 3\) and \(\lambda = 480 \mathrm{nm}\), into the formula gives the path difference.

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Key Concepts

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

Intensity Calculation
In two-slit interference, the intensity pattern forms due to the constructive and destructive interactions of light waves from both slits. To find the intensity at a specific point in the pattern, we use the formula:
  • \( I = I_{0} \cos^{2}(\phi / 2) \)
Here,
  • \(I\) is the intensity at the point,
  • \(I_{0}\) is the peak intensity at the central maximum,
  • \(\phi\) is the phase difference in radians.

To solve the problem, first convert the phase difference from degrees to radians since trigonometric functions require radians. For \(60^{\circ}\), the conversion is \(\phi = \pi / 3\). Then, substitute
  • \(\phi = \pi / 3\) (radians)
into the equation to calculate
  • the intensity \(I\).
  • Calculate \(I = I_{0} \cos^{2}(\pi / 6)\). Since
    • \(\cos(\pi / 6) = \sqrt{3}/2\),

    we find \(I = I_{0} (3/4)\).
    Thus, at \(60^{\circ}\), the intensity is three-fourths (or 75%) of the peak intensity \(I_{0}\).
    Phase Difference
    Phase difference (\(\phi\)) measures how "out of step" or "in step" waves from the two slits are with each other. It’s crucial in determining where peaks and troughs in the interference pattern occur. The formula used here helps calculate the intensity by
    • relating \(\phi\) to the position within the fringe pattern.
    phase difference \(\phi\) is determined by factors like
    path difference and wavelength. It is typically expressed in radians for calculations involving trigonometric functions. In this problem, the given phase difference is initially \(60^{\circ}\), which means that the path of one wave is ahead of the other by that angle. Transforming this into radians yields
    • \(\phi = \pi / 3\)

    for further use in calculations. This conversion is essential since trigonometric functions, like cosine, require radian measures to calculate associated intensities or displacements.
    Path Difference
    Path difference refers to the physical length difference between the paths traveled by two waves from their respective slits to a common point. This difference dictates the phase difference (\(\phi\)) and thus the interference pattern formed.
    The formula for path difference is:
    • \(d = \lambda \phi / (2\pi)\),
    where
    • \(d\) is the path difference,
    • \(\lambda\) is the wavelength of the light,
    • \(\phi\) is the phase difference in radians.
    In the context of this problem, substituting the given values into the formula
    • (\(\phi = \pi / 3\), and \(\lambda = 480 \text{ nm}\))

    enables you to find the path difference. This computes to
    • \(d = 480 \text{ nm} \times \pi / 3 / (2\pi) = 80 \text{ nm}\).
    Thus, the path difference where the phase difference is \(60^{\circ}\) in the interference pattern is
    • 80 nm.
    Wavelength of Light
    The wavelength of light (\(\lambda\)) is a fundamental property dictating how light waves propagate and interfere. It is defined as the distance between successive crests (or troughs) of a wave and is key to understanding interference phenomena.
    In calculations involving interference, the wavelength helps determine both path and phase differences. It plays a part in calculating path differences since changes in wavelength will affect the distance the waves must travel to recombine constructively or destructively.
    In this exercise, the wavelength
    • \(\lambda = 480 \text{ nm}\)

    is critical in computing the path difference required for a given phase difference. The relationship between wavelength and both path and phase differences allows us to describe entire interference phenomena and predict where constructive or destructive interference will occur in the pattern.

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    Most popular questions from this chapter

    Coherent light of frequency \(6.32 \times 10^{14} \mathrm{~Hz}\) passes through two thin slits and falls on a screen \(85.0 \mathrm{~cm}\) away. You observe that the third bright fringe occurs at \(\pm 3.11 \mathrm{~cm}\) on either side of the central bright fringe. (a) How far apart are the two slits? (b) At what distance from the central bright fringe will the third dark fringe occur?

    Two slits spaced \(0.260 \mathrm{~mm}\) apart are \(0.900 \mathrm{~m}\) from a screen and illuminated by coherent light of wavelength \(660 \mathrm{nm}\). The intensity at the center of the central maximum \(\left(\theta=0^{\circ}\right)\) is \(I_{0} .\) What is the distance on the screen from the center of the central maximum (a) to the first minimum; (b) to the point where the intensity has fallen to \(I_{0} / 2 ?\)

    A plastic film with index of refraction 1.70 is applied to the surface of a car window to increase the reflectivity and thus to keep the car's interior cooler. The window glass has index of refraction \(1.52 .\) (a) What minimum thickness is required if light of wavelength \(550 \mathrm{nm}\) in air reflected from the two sides of the film is to interfere constructively? (b) Coatings as thin as that calculated in part (a) are difficult to manufacture and install. What is the next greater thickness for which constructive interference will also occur?

    Jan first uses a Michelson interferometer with the \(606 \mathrm{nm}\) light from a krypton-86 lamp. He displaces the movable mirror away from him, counting 818 fringes moving across a line in his field of view. Then Linda replaces the krypton lamp with filtered \(502 \mathrm{nm}\) light from a helium lamp and displaces the movable mirror toward her. She also counts 818 fringes, but they move across the line in her field of view opposite to the direction they moved for Jan. Assume that both Jan and Linda counted to 818 correctly. (a) What distance did each person move the mirror? (b) What is the resultant displacement of the mirror?

    White light reflects at normal incidence from the top and bottom surfaces of a glass plate \((n=1.52) .\) There is air above and below the plate. Constructive interference is observed for light whose wavelength in air is \(477.0 \mathrm{nm}\). What is the thickness of the plate if the next longer wavelength for which there is constructive interference is \(540.6 \mathrm{nm} ?\)

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