Optical power lost at a pinhole

  • Context: Undergrad 
  • Thread starter Thread starter lalligagger
  • Start date Start date
  • Tags Tags
    Lost Optical Power
Click For Summary
SUMMARY

The discussion focuses on modeling optical power loss at a pinhole in a solar spectrometer design. The user proposes a formula involving solar intensity, aperture area, and pinhole area to calculate power transmission. Key considerations include the use of an ideal lens and the Airy function to describe light distribution at the focal plane. The width of the Airy disk, determined by the lens's wavelength and f-number, is crucial for comparing with the pinhole size to assess power loss.

PREREQUISITES
  • Understanding of optical physics, specifically light propagation and lens behavior.
  • Familiarity with the Airy function and its application in optics.
  • Knowledge of solar intensity and its measurement.
  • Basic principles of geometrical optics, including focal length and aperture concepts.
NEXT STEPS
  • Research the Airy disk and its implications in optical systems.
  • Study the impact of f-number on lens performance and light gathering.
  • Explore methods for optimizing pinhole size in optical instruments.
  • Investigate solar intensity measurements and their relevance in spectrometer design.
USEFUL FOR

Physics undergraduates, optical engineers, and researchers involved in designing and optimizing spectrometers or similar optical systems.

lalligagger
Messages
14
Reaction score
0
Hi,
I am a physics undergrad designing a solar spectrometer as part of a senior design type course. If we have light incident from the sun onto some sort of telescope objective (say a single lens for simplicity, focal length "f" and aperture radius "R") and then a pinhole at the focal point (radius "r"), how do we model the power loss at the pinhole? I was thinking it'd be
Isun*(pi*R2)*[(.01*f/2)2/(r)2]
In other words, intensity times the area of the entrance aperture gives you power in, and taking the ratio of your image area over the pinhole area gives you the fraction of power that gets through. The .01 comes from the sun being approximately .01 radians in the sky. This made sense to me, but it seems like we would barely get any power through with a 1 meter telescope into a 20-50 micron pinhole. Any help would be greatly appreciated.
 
Science news on Phys.org
For an ideal lens used the way you are thinking (object at infinity), the distribution of light at the focal plane is given by an Airy function, which can be written as J_1(ax)/ax, just like sinc(ax) = sin(ax)/ax.

The width of the Airy disk is given by the wavelength and f-number (or numerical aperture) of the lens:

http://en.wikipedia.org/wiki/Airy_disk

For your application, simply compare the size of the Airy disk with the size of the pinhole.
 

Similar threads

  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 25 ·
Replies
25
Views
4K
  • · Replies 7 ·
Replies
7
Views
4K
  • · Replies 1 ·
Replies
1
Views
4K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 7 ·
Replies
7
Views
1K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 6 ·
Replies
6
Views
4K
  • · Replies 4 ·
Replies
4
Views
1K