The diffraction limit of the Hubble ST

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SUMMARY

The diffraction limit of the Hubble Space Telescope (HST) is calculated using the formula θ = 1.22 λ/D, where λ is the wavelength of light (500 nm) and D is the diameter of the objective lens (2.5 m). The choice of 500 nm is justified as it coincides with the sensitivity peak of the human eye and the middle of the visible spectrum, despite the HST using CCD sensors. The diffraction limit varies with wavelength, and while the HST can achieve an angular resolution of approximately 0.05 arcseconds at 500 nm, it can theoretically perform better in the 380-450 nm range. The discussion highlights the limitations of using a single wavelength for calculating diffraction limits in optical telescopes.

PREREQUISITES
  • Understanding of the diffraction limit formula θ = 1.22 λ/D
  • Familiarity with the Hubble Space Telescope's specifications, including its 2.5 m objective lens
  • Knowledge of light wavelengths, particularly in the visible spectrum (380-750 nm)
  • Basic principles of optics and CCD sensor technology
NEXT STEPS
  • Research the impact of different wavelengths on the diffraction limit of telescopes
  • Explore the specifications and performance of Hubble's various cameras, including WFPC2
  • Learn about the significance of the Sodium D line (532 nm) in optical measurements
  • Investigate the relationship between angular resolution and detector capabilities in astronomical imaging
USEFUL FOR

Astronomers, optical engineers, and students studying astrophysics or optical systems will benefit from this discussion, particularly those interested in the performance and limitations of the Hubble Space Telescope.

TheMan112
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I'm trying to calculate the diffraction limit/angular resolution for the Hubble Space Telescope. I know this can be found using the formula:

\theta = 1.22 \frac{\lambda}{D}

Where \lambda is the wavelength of the light being observed and D is the diameter of the objective lens (2.5 m on Hubble).

Now since Hubble is able to observe a wade range of wavelenghts from the ultraviolet to the visible to the infrared spectrum I would describe the diffraction limit as an interval depeding on this range of wavelenghts.

However, in all examples I've been able to find, even http://www.nasa.gov/missions/highlights/webcasts/shuttle/sts109/hubble-qa.html" , the diffraction limit of optical telescopes is calculated using a single wavelength of 500 nm (~cyan). What's the justification for using this particular wavelength for Hubble (and other optical telescopes).

500 nm coincides with:

1. The irradience top of sunlight (and thus any G-type star). See: http://en.wikipedia.org/wiki/File:EffectiveTemperature_300dpi_e.png
2. The sensitivity top of the human eye.
3. The approximate middle wavelength of the visible spectrum.

However (respectively):

1. G-type stars aren't all that common, comprising only 7.6% of all stars, thus the usage is limited and this point cannot be applied to all visible starlight.
2. The HST employs CCD sensors and not direct human observation, thus point 2 is irrelevant.
3. This is the only point that seems relevant. However the HST would theoretically achieve greater angular resolution by using say the 380-450 nm range.

So what's the point of using 500 nm when calculating the diffraction limit?
 
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For optics you tradiationaly use the Sodium D line (532nm) because before lasers it was the easiest bright monochromatic source.
The diffraction limit of the HST is different at each wavelength, the optics aren't necessarily diffraction limited at all wavelengths or the detectors have enough resolution to sample the diffraction limit.
 
Yeah, it apprears the detectors on WFPC2 can resolve down to 0.04 arcsec, given that lamda = 500 nm we get an angular resolution for the telescope itself at roughly 0.05 arcsec. The other camera appears to have much worse resolutions. Thanks!
 

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