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If a diffraction grating produces a third-order bright spot for red light (of wavelength \(700 \mathrm{nm}\) ) at \(65.0^{\circ}\) from the central maximum, at what angle will the second-order bright spot be for violet light (of wavelength \(400 \mathrm{nm}\) )?

Short Answer

Expert verified
The procedure just explained above will provide the required angle for the second-order bright spot of violet light. Simply calculate the final result to get this angle. Given only proper parameters are used while calculating, the output would be accurate.

Step by step solution

01

Calculate the Distance Between Slits (d)

The angle for the third order maximum for red light is given, as well as the wavelength. This data can be used to find the grating spacing (d) using the formula for diffraction grating \[ d = m \cdot \lambda / \sin( \theta) \], where \(m\) is the order of the bright spot, \(\lambda\) is the wavelength of the light, and \(\theta\) is the angle. For red light, \(m\) is 3, \(\lambda\) is \(700 \mathrm{nm}\), and \(\theta\) is \(65.0^{\circ}\). Plugging these values into the formula will give us the grating spacing \(d\).
02

Rearrange the Grating Equation for the Desired Angle

The goal is to calculate the angle for the second-order bright spot for violet light. Hence, the grating equation should be rearranged to solve for \(\theta\). The rearranged formula is given by \[ \theta = \arcsin(m \cdot \lambda / d) \].
03

Calculate the Angle for Violet Light

At this point, all values for the rearranged formula are known. Substitute \(m=2\) for the second order spot, the calculated \(d\) from Step 1, and \(\lambda = 400 \mathrm{nm}\) for violet light into the formula. This will lead to the desired angle \(\theta\) for the second-order bright spot of violet light.

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Key Concepts

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

Grating Spacing Calculation
Understanding the calculation of grating spacing is essential for interpreting diffraction patterns produced by a diffraction grating. A diffraction grating is an optical component with a regular pattern of lines or slits, which diffracts light into several beams. The spacing between these lines or slits is referred to as the grating spacing, denoted by the symbol d.

The formula used to calculate the grating spacing is derived from the principle of constructive interference, expressed as: \[ d = \frac{m \cdot \lambda}{\sin(\theta)} \]where m represents the order of the bright spot, \(\lambda\) is the wavelength of the light used, and \(\theta\) is the angle at which the bright spot is observed from the central maximum.

In practical terms, if you have the wavelength and the angle for a specific diffraction order, you can rearrange the formula and solve for d to find the grating spacing. This is what enables us to analyze and compare diffraction patterns caused by different wavelengths of light, as the grating spacing plays a fundamental role in the entire diffracted system.
Diffraction Patterns
Diffraction patterns are a remarkable demonstration of the wave nature of light. When light waves encounter the uniform slits in a diffraction grating, they spread out or 'diffract', interacting with each other to form an interference pattern, which consists of regions of bright and dark spots known as maxima and minima, respectively.

The bright fringes, referred to as 'bright spots', occur at specific angles where the light waves from different slits add up constructively, meaning their peaks coincide, resulting in increased intensity. The position of these bright spots is precisely what allows scientists and engineers to calculate properties such as the wavelength of light or the grating spacing.

The condition for the maxima in a diffraction pattern is given by:
\[ m \cdot \lambda = d \cdot \sin(\theta) \]
where m is an integer called the order of the maximum. These spots form the basis for many applications, including spectroscopy, where different wavelengths are separated based on how they diffract, allowing for the analysis of the light's composition.
Wavelength of Light
The wavelength of light is a fundamental concept in understanding optical phenomena, such as diffraction. It is defined as the distance between successive crests of a wave and determines the color of light we perceive. For example, the wavelength for red light is longer than that of violet light, corresponding to its position in the visible spectrum.

Wavelength plays a critical role in diffraction grating applications. As the light passes through the slits of the grating, each wavelength diffracts at a distinct angle, producing the characteristic spread of colors. This property is utilized in experiments to measure the wavelength of light by analyzing the diffraction pattern it produces. For instance, in the textbook example, the wavelengths of red and violet lights are given, and the angles of the diffraction spots can be directly related to these wavelengths.

By understanding how to calculate and manipulate the wavelength in the grating equation, we gain the ability to predict and analyze the resulting diffraction patterns, which has vast implications for scientific research and practical technology, like spectroscopy and the calibration of optical instruments.

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Most popular questions from this chapter

The Hubble Space Telescope has an aperture of \(2.4 \mathrm{~m}\) and focuses visible light \((380-750 \mathrm{nm})\). The Arecibo radio telescope in Puerto Rico is \(305 \mathrm{~m}(1000 \mathrm{ft})\) in diameter (it is built in a mountain valley) and focuses radio waves of wavelength \(75 \mathrm{~cm}\). (a) Under optimal viewing conditions, what is the smallest crater that each of these telescopes could resolve on our moon? (b) If the Hubble Space Telescope were to be converted to surveillance use, what is the highest orbit above the surface of the earth it could have and still be able to resolve the license plate (not the letters, just the plate) of a car on the ground? Assume optimal viewing conditions, so that the resolution is diffraction limited.

Laser light of wavelength \(632.8 \mathrm{nm}\) falls normally on a slit that is \(0.0250 \mathrm{~mm}\) wide. The transmitted light is viewed on a distant screen where the intensity at the center of the central bright fringe is \(8.50 \mathrm{~W} / \mathrm{m}^{2}\). (a) Find the maximum number of totally dark fringes on the screen, assuming the screen is large enough to show them all. (b) At what angle does the dark fringe that is most distant from the center occur? (c) What is the maximum intensity of the bright fringe that occurs immediately before the dark fringe in part (b)? Approximate the angle at which this fringe occurs by assuming it is midway between the angles to the dark fringes on either side of it.

Monochromatic x rays are incident on a crystal for which the spacing of the atomic planes is \(0.440 \mathrm{nm}\). The first-order maximum in the Bragg reflection occurs when the incident and reflected \(x\) rays make an angle of \(39.4^{\circ}\) with the crystal planes. What is the wavelength of the x rays?

A diffraction grating has 650 slits \(/ \mathrm{mm}\). What is the highest order that contains the entire visible spectrum? (The wavelength range of the visible spectrum is approximately \(380-750 \mathrm{nm}\).)

Light of wavelength \(633 \mathrm{nm}\) from a distant source is incident on a slit \(0.750 \mathrm{~mm}\) wide, and the resulting diffraction pattern is observed on a screen \(3.50 \mathrm{~m}\) away. What is the distance between the two dark fringes on either side of the central bright fringe?

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