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The second-order maximum produced by a diffraction grating with 560 lines per centimeter is at an angle of \(3.1^{\circ}\). (a) What is the wavelength of the light that illuminates the grating? (b) If a grating with a larger number of lines per centimeter is used with this light, is the angle of the second-order maximum greater than or less than \(3.1^{\circ}\) ? Explain.

Short Answer

Expert verified
(a) \( \lambda \approx 482 \) nm. (b) The angle is greater than \( 3.1^{\circ} \).

Step by step solution

01

Convert lines per cm to lines per meter

The diffraction grating has 560 lines per centimeter. To convert this to lines per meter, multiply by 100 (since there are 100 centimeters in a meter): \( 560 \times 100 = 56,000 \) lines per meter. This gives the grating spacing, \( d \), as the reciprocal: \( d = \frac{1}{56,000} \) m.
02

Use the diffraction grating equation

The diffraction grating equation is \( d \sin \theta = m \lambda \), where \( d \) is the spacing between lines, \( \theta \) is the angle of the diffraction order, \( m \) is the order of the maximum, and \( \lambda \) is the wavelength. Given: \( d = \frac{1}{56,000} \) m, \( \theta = 3.1^{\circ} \), \( m = 2 \). We want to solve for \( \lambda \).
03

Calculate \( \lambda \)

Substitute the values into the diffraction equation: \( \frac{1}{56,000} \times \sin(3.1^{\circ}) = 2 \lambda \). Calculate \( \sin(3.1^{\circ}) \approx 0.054 \). Thus, \( \frac{1}{56,000} \times 0.054 = 2 \lambda \). Solving for \( \lambda \), we find \( \lambda \approx \frac{0.054}{2 \times 56,000} \approx 4.82 \times 10^{-7} \) m or 482 nm.
04

Analyze the effect of a larger number of lines per cm

If the number of lines per centimeter increases, \( d \) (the spacing between lines) decreases. Since \( d \sin \theta = m \lambda \), a smaller \( d \) for the same wavelength \( \lambda \) requires \( \sin \theta \) (and hence \( \theta \)) to increase to maintain the equality. Thus, the angle \( \theta \) for the second-order maximum must be greater than \( 3.1^{\circ} \).

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Key Concepts

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

Wavelength
In the context of diffraction gratings, the wavelength is a critical concept. The wavelength (\( \lambda \)) is the distance between successive peaks of a wave.
In the exercise we are solving, we are dealing with light waves. Light, like all waves, is characterized by its wavelength, which determines its color.
In this case, the light passing through the diffraction grating is calculated to have a wavelength of 482 nm, which is in the visible spectrum.Wavelength is key because it affects how light behaves when it encounters obstacles or openings.
  • When light hits a diffraction grating, the spread of the light will change depending on its wavelength.
  • Longer wavelengths result in a wider spread and shorter wavelengths result in a narrower spread when passing through a diffraction grating.
Understanding the wavelength also helps us determine other variables, such as the angle of diffraction and the grating spacing in diffraction experiments.
Angle of Diffraction
The angle of diffraction (\( \theta \)) in a diffraction grating experiment is the angle at which light is scattered by the grating.
It is measured from the incidence direction.
In our exercise, the second-order maximum appears at an angle of 3.1 degrees.The angle of diffraction is important because it shows how the light is dispersed based on its wavelength and the grating's properties.
  • According to the diffraction grating equation (\( d \sin \theta = m \lambda \)), the angle of diffraction depends on the wavelength, the order of diffraction, and the grating spacing.
  • A larger wavelength or a higher order will increase the angle, resulting in more spread of light.
Additionally, the angle of diffraction changes if the grating spacing changes. For example, using a more finely spaced grating with the same light will result in a larger angle of diffraction.
Grating Spacing
Grating spacing (\( d \)) refers to the distance between adjacent lines on a diffraction grating.
It's the inverse of the number of lines per meter.
In the initial example, 560 lines per centimeter translates to 56,000 lines per meter, which means our grating spacing is \( d = \frac{1}{56,000} \) meters.This spacing is crucial for determining how the grating will affect light passing through it.
  • The closer the lines are together (smaller \( d \)), the more the light spreads out.
  • The relationship between grating spacing and the angle of diffraction is direct. With smaller spacing, each wavelength bends more, resulting in larger angles of diffraction.
As shown in the solution, reducing the grating spacing increases the angle of diffraction necessary to achieve higher orders of maximum, given the same wavelength.
Thus, the choice of grating spacing is essential for specific applications, determining how effectively certain wavelengths will be diffracted.

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Most popular questions from this chapter

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