Astronomy 3520: Grating Review Sheet

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For a reflection grating, nλ = d(sin α ± sin β), where α and β are the incident and reflected angles respectively

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For a transmission grating, however, nλ = d sin θ because we assume the incident angle is 0.

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To derive the resolution of a telescope, we start with the dispersion equation nλ = d sin θ

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We also know that dθ = "gratingreview_7.gif"where x is the size of the image on your focal plane (in general, you probably want your smallest resolution element to be nyquist sampled, so x should be twice the pixel size) and "gratingreview_8.gif" is the focal length of your camera optics.  This can be recovered from our familiar diagram:

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where in this case, the size on the focal plane is x, the focal length is the camera focal length, and θ is dθ

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In the calculations below, all units will be centimeters

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What if we had been given a different value?  Say we knew the central wavelength λ = 4400 Å instead of the angle θ :

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So the resolution is higher (3000), but our camera has to be at an angle of 45 degrees instead of 35 degrees for the first order


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