Exam 36: Diffraction

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600-nm light is incident on a defraction grating with a ruling separation of 1.7*10-6 m. The second order line occurs at a diffraction angle of:

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At a diffraction line phasors associated with waves from the slits of a multiple-slit barrier:

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Two nearly equal wavelengths of light are incident on an N slit grating. The two wavelengths are not resolvable. When N is increased they become resolvable. This is because:

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A diffraction grating just resolves the wavelengths 400.0 nm and 400.1 nm in first order. The number of slits in the grating is:

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A student wishes to produce a single-slit diffraction pattern in a ripple tank experiment. He considers the following parameters: A student wishes to produce a single-slit diffraction pattern in a ripple tank experiment. He considers the following parameters:   Which two of the above should be decreased to produce more bending? Which two of the above should be decreased to produce more bending?

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Sound differs from light in that sound:

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What is the minimum number of slits required in a deffraction grating to just resolve light with wavelengths of 471.0 nm and 471.6 nm?

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Bragg's law for x-ray diffraction is 2d sin θ\theta = m λ\lambda , where θ\theta is the angle between the incident beam and:

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In order to obtain a good single-slit diffraction pattern, the slit width could be:

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X rays are:

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In a single-slit diffraction pattern, the central maximum is about twice as wide as the other maxima. This is because:

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A beam of x-rays of wavelength 0.20 nm is diffracted by a set of planes in a crystal whose separation is 3.1* 10-8 cm. The smallest angle between the beam and the crystal planes for which a reflection occurs is:

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A diffraction grating of width W produces a deviation θ\theta in second order for light of wavelength λ\lambda . The total number N of slits in the grating is given by:

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In the equation d sin θ\theta = m λ\lambda for the lines of a diffratction grating m is:

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A diffraction-limited laser of length  A diffraction-limited laser of length   and aperture diameter d generates light of wavelength  \lambda . If the beam is directed at the surface of the Moon a distance D away, the radius of the illuminated area on the moon is approximately: and aperture diameter d generates light of wavelength λ\lambda . If the beam is directed at the surface of the Moon a distance D away, the radius of the illuminated area on the moon is approximately:

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In the equation sin θ\theta = λ\lambda /a for single-slit diffraction, θ\theta is:

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Figure (i) shows a double-slit pattern obtained using monochromatic light. Consider the following five possible changes in conditions: Figure (i) shows a double-slit pattern obtained using monochromatic light. Consider the following five possible changes in conditions:   Which of the above would change Figure (i) into Figure (ii)?  Which of the above would change Figure (i) into Figure (ii)? Figure (i) shows a double-slit pattern obtained using monochromatic light. Consider the following five possible changes in conditions:   Which of the above would change Figure (i) into Figure (ii)?

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Radio waves are readily diffracted around buildings whereas light waves are negligibly diffracted around buildings. This is because radio waves:

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As more slits with the same spacing are added to a multiple-slit system the lines:

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The largest x-ray wavelength that can be diffracted by crystal planes with a separation of 0.316 nm is:

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