Astronomy 3520: Grating Review Sheet
For a reflection grating, nλ = d(sin α ± sin β), where α and β are the incident and reflected angles respectively
For a transmission grating, however, nλ = d sin θ because we assume the incident angle is 0.
To derive the resolution of a telescope, we start with the dispersion equation nλ = d sin θ
We also know that dθ =
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
is the focal length of your camera optics. This can be recovered from our familiar diagram:
where in this case, the size on the focal plane is x, the focal length is the camera focal length, and θ is dθ
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
| Created by Wolfram Mathematica 6.0 (08 November 2007) |