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(A) sinλ = 1.22 λ /d
λ = sin-1 (1.22 ? /d ) .................(1)
Here d = diametre of the pin hole = 0.1*10-3 m
wave length λ = 632.8*10-9 m
λ = 0.4420m
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(B) when λ is small
tanλ = sin? = y / L
Radius of the first dark fringe y = Ltan? = ( 3m )( tan 0.4420 ) =
0.023.2 m = 23.2 mm
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(C) Area = pi2 = 3.14 ( 0.023.2 m ) 2 = 1690.0736( mm)2
The first dark ring forms the boundary for the bright Airy disk at the center of the diffraction pattern. What is the a...
I have Part C and E left ??how to do it ? Consider light from a helium-neon laser (λ=632.8 nanometers) striking a pinhole with a diameter of 0.160 mm . Part A At what angle θ1 to the normal would the first dark ring be observed? θ1 = 0.276 ∘ Correct Part B Suppose that the light from the pinhole projects onto a screen 3.00 meters away. What is the radius r1 of the first dark ring on that screen?...
Learning Goal: To use the formulas for the locations of the dark bands and understand Rayleigh's criterion of resolvability.An important diffraction pattern in many situations is diffraction from a circular aperture. A circular aperture is relatively easy to make: all that you needis a pin and something opaque to poke the pin through. The figure shows a typical pattern. It consists of a bright central disk, called the Airy disk,surrounded by concentric rings of dark and light.While the mathematics required...
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Part A: At what angle θ1 to the normal would the first dark ring be observed? answer is .442o Part B: Suppose that the light from the pinhole projects onto a screen 3 meters away. What is the radius of the first dark ring on that screen? Notice that the angle from Part A is small enough that sinθ≈tanθ . Answer is 23.2mm Part C: The first dark ring forms the boundary for the bright Airy disk at the center of...
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