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Principal Maxima

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College Physics I – Introduction

Definition

In the context of single slit diffraction, the principal maxima refer to the bright interference patterns observed at specific angular positions where the diffracted light constructively interferes. These principal maxima occur at the angles where the path difference between adjacent wavelets from the slit is an integer multiple of the wavelength.

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5 Must Know Facts For Your Next Test

  1. The principal maxima in single slit diffraction occur at angles where the path difference between adjacent wavelets is an integer multiple of the wavelength (n\lambda, where n is an integer).
  2. The angular positions of the principal maxima are given by the formula \theta_n = \sin^{-1}(n\lambda/a), where a is the width of the slit and \lambda is the wavelength of the light.
  3. The central principal maximum, also known as the central bright fringe, occurs at \theta_0 = 0, where the path difference is zero and the waves constructively interfere.
  4. The intensity of the principal maxima decreases as the order n increases, with the first-order maxima being the brightest after the central maximum.
  5. The spacing between the principal maxima is inversely proportional to the slit width a, meaning a narrower slit will result in a larger angular separation between the maxima.

Review Questions

  • Explain the relationship between the path difference and the angular positions of the principal maxima in single slit diffraction.
    • The principal maxima in single slit diffraction occur at the angles where the path difference between adjacent wavelets from the slit is an integer multiple of the wavelength (n\lambda, where n is an integer). This path difference determines the constructive interference pattern, with the central maximum occurring at \theta_0 = 0 where the path difference is zero, and the higher-order maxima occurring at angles given by \theta_n = \sin^{-1}(n\lambda/a), where a is the slit width. The spacing between the principal maxima is inversely proportional to the slit width, as a narrower slit results in a larger angular separation between the maxima.
  • Describe how the intensity of the principal maxima changes as the order n increases in single slit diffraction.
    • In single slit diffraction, the intensity of the principal maxima decreases as the order n increases. The central principal maximum, or central bright fringe, is the brightest, and the intensity of the higher-order maxima diminishes with increasing n. This is because the path difference between adjacent wavelets increases with higher orders, leading to a smaller fraction of the wavefront contributing to the constructive interference at those angles. As a result, the principal maxima become less pronounced and the overall diffraction pattern becomes more complex as the order n increases.
  • Analyze how the slit width a affects the angular separation between the principal maxima in single slit diffraction.
    • In single slit diffraction, the angular separation between the principal maxima is inversely proportional to the slit width a. This means that a narrower slit will result in a larger angular separation between the maxima, while a wider slit will have a smaller angular separation. This relationship is expressed in the formula \theta_n = \sin^{-1}(n\lambda/a), where \theta_n is the angle of the n-th principal maximum, \lambda is the wavelength of the light, and a is the slit width. By decreasing the slit width a, the denominator in the formula becomes smaller, leading to a larger angle \theta_n and a greater separation between the principal maxima. This is an important consideration in the design of optical devices that rely on diffraction, as the slit width can be adjusted to control the angular spacing of the diffraction patterns.

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