How Does Light Intensity Vary with Distance from an Incoherent Extended Source?

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The discussion focuses on understanding how light intensity varies with distance from an incoherent extended source. The user is exploring the problem by modeling it similarly to electrostatics, considering a line of infinitesimal sources contributing light to a point. They mention using a Lambertian emitter model and integrating over the entire source, but encounter complex expressions in their calculations. Suggestions include considering the far-field diffraction pattern for an aperture shaped like the source, as it relates to incoherent fields. The conversation emphasizes the need for a clearer approach and resources for studying extended sources in optics.
reasonableman
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I'm currently trying to look into the optics of extended sources. Google doesn't seem too helpful.

Anyway, I have just been thinking about it and thought that surely one of the easiest problems would be the intensity at a screen at a particular distance from an incoherent, spatial extended source.

To me it looks pretty much like an electrostatics problem, common as an undergraduate.

I'm envisioning a line of infinitesimal sources, which will each contribute some light to a point. Which assuming a Lambertian emitter will be the intensity of that infinitesimal point but taking into account the 1/r^2 drop off and the cosine of the angle of the point.

I then integrate over the whole source. However when I put this into maxima (can't do it manually) I get some horrendously long expressions.

Am I doing something wrong with my model and can anyone suggest an introductory text for extended sources?
 
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It is covered in many optics courses, but disguised. In fact, what you are asking is the far-field diffraction pattern for an aperture, when the field aperture is not a (coherent) plane wave but an incoherent field, and the aperture is shaped like your source. Try that approach and see what happens.
 
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