Question about optics (diffraction)

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SUMMARY

The discussion centers on the phenomenon of diffraction in optics, specifically how the size of a hole affects the resulting projection pattern on a screen. As the hole size decreases, the pattern initially shrinks before expanding again. The user seeks to derive a formula for the screen pattern diameter based on the hole size, distance to the screen, and wavelength. The Kirchhoff integral theorem is mentioned as a potential method for this derivation, although the user questions its complexity.

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  • Understanding of diffraction principles in optics
  • Familiarity with the Kirchhoff integral theorem
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Gza
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I was working out a practice test on optics and was a little confused about how to tackle this problem:


If you illuminate a hole and project the resulting pattern on a screen- as you decrease the hole size, the screen pattern gets smaller initially and then ultimately begins to grow larger. Why is this? Derive a formula for the screen pattern diameter as a function of the hole size, distance between screen and hole and the wavelength.


I know the effect is diffraction, but deriving the mentioned relation is giving me trouble. I was thinking of using the kirchhoff integral theorem, and then perhaps carrying out an integral over a rectangular aperature; but maybe that is overkill. Is their an easier way to start thinking about this?
 
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Gza said:
If you illuminate a hole and project the resulting pattern on a screen- as you decrease the hole size, the screen pattern gets smaller initially and then ultimately begins to grow larger. Why is this? Derive a formula for the screen pattern diameter as a function of the hole size, distance between screen and hole and the wavelength.
Is this considered introductory physics nowadays? :eek: I must be getting old.

Maybe this will help a bit:
http://en.wikipedia.org/wiki/Diffraction
 
Lol, yeah this was probably a mispost; i got a chance to check the other posts in this section and realized it at that point. Thanks for the reference though galileo.
 

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