Interference/Difraction wrong consideration

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SUMMARY

The discussion addresses the misconception regarding the intensity of the middle fringe in diffraction patterns, specifically challenging the assumption that it is N times the intensity of individual light sources. It asserts that this assumption neglects phase differences between light beams emitted from multiple sources, particularly when the slit size significantly exceeds the wavelength. For example, with a wavelength of 1000nm and a slit size of 1mm, the intensity calculated is I = 0.88 I0, indicating a substantial deviation from the expected intensity. The conversation emphasizes the need for careful consideration of diffraction principles, particularly in relation to Fraunhofer and Fresnel diffraction.

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jaumzaum
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Every difraction/multiple slit article I've read until now consider the intensity of the middle fringe to be N times the intensity of the single light sources (in difraction I've divided the slit into n small light sources, that means that N.I0 = I = the intensity of the light reaching the whole slit).

This statement in completelly wrong! It consider that all light beams emmited by each light source does not have a phase difference! This would be a good aproximation if we consider the slit size d to be aproximatelly equal to the wave lenght. But it would still be a aproximation. What if the slit size were very bigger than the wave lenght? Let's say a λ=1000nm, d=1mm and L (distance of the screen to the slit) = 1m. This would give
I = 0.88 I0
The result would be very smaller if d = 2, 3 or 10mm
And all those numbers are plausible (the example I calculated λ=1000nm, d=1mm and L= 1m is even in Tipler's book)

http://img22.imageshack.us/img22/5834/sadgdfgdg.png


The path difference is
θ=[itex](\sqrt{L^{2}+x^{2}}-L)*2\pi/\lambda[/itex]

So we have to integrate Sin[θ] from {x, -d/2, d/2}. The problem is that this integral have to be aproximated. A small aprox for the amplitude A is A0 times

http://img803.imageshack.us/img803/3166/sdgfghg.png


So why the books insist to say the intensity does not change?
 
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You are right to be concerned about this but it is not always relevant.
For a narrow aperture or array of sources and a long throw (L), that simple assumption is accurate enough to make the approximation. Look up Fraunhoffer and Fresnel Diffraction to see this discussed in high or low detail - depending on what you want. Here is one link which discusses the problem.
In some cases there is a further consideration and that is that the elements in an array of diffracting sources may not all even 'point' in the same direction; they may not even be considered as point (omnidirectional) sources. Arrays of radio antennae often have non-parallel elements but then, one is more likely to be considering the Fraunhoffer region rather than the near field.
 

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