If you can read the bottom row of your doctor’s eye chart, your eye has a resolving power of 1 arcminute, equal to 1/60 degree. If this resolving power is diffraction-limited, to what effective diameter of your eye’s optical system does this correspond? Use Rayleigh’s criterion and assume λ = 550 nm.
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34. Wave Optics
Diffraction
Problem 47
Textbook Question
(III) The yellow sodium D lines have wavelengths of 589.0 and 589.6 nm. When they are used to illuminate a Michelson interferometer, it is noted that the interference fringes disappear and reappear periodically as the mirror M₁ is moved. Why does this happen? How far must the mirror move between one disappearance and the next?

1
The Michelson interferometer works by splitting a beam of light into two paths, reflecting them back, and recombining them to produce interference patterns. The interference depends on the path difference between the two beams.
The sodium D lines consist of two closely spaced wavelengths, λ₁ = 589.0 nm and λ₂ = 589.6 nm. When these two wavelengths interfere, they produce a beat pattern due to their slightly different frequencies. This beat pattern causes the interference fringes to periodically disappear and reappear.
The condition for the disappearance of fringes is when the path difference between the two beams corresponds to a phase difference of 2π for one wavelength and an integer multiple of 2π for the other wavelength. This happens when the path difference matches the least common multiple of the wavelengths' beat frequency.
The beat wavelength, λ_beat, is given by the formula: , where Δλ = λ₂ - λ₁. Substituting the values, calculate λ_beat to find the effective wavelength of the beat pattern.
The mirror must move by half the beat wavelength, , between one disappearance and the next. This is because the path difference changes by twice the mirror movement in a Michelson interferometer.

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Key Concepts
Here are the essential concepts you must grasp in order to answer the question correctly.
Interference
Interference is a phenomenon that occurs when two or more waves overlap and combine to form a new wave pattern. In the context of light, constructive interference occurs when waves are in phase, enhancing brightness, while destructive interference occurs when they are out of phase, leading to darkness. This principle is fundamental in understanding how the Michelson interferometer works, as it relies on the interference of light waves from two paths.
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Michelson Interferometer
The Michelson interferometer is an optical instrument used to measure the interference of light waves. It splits a beam of light into two paths, reflects them back, and then recombines them. The resulting interference pattern can be analyzed to determine changes in distance or wavelength, making it a powerful tool in precision measurements and experiments in physics.
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Wavelength and Path Difference
Wavelength is the distance between successive peaks of a wave, and it plays a crucial role in interference patterns. In the case of the sodium D lines, the two wavelengths (589.0 nm and 589.6 nm) create a situation where the path difference between the two beams must equal an integer multiple of the wavelengths for constructive interference to occur. The distance the mirror must move to cause a disappearance and reappearance of fringes is half the wavelength of the light used, as this corresponds to a full cycle of constructive and destructive interference.
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