Two slit diffraction and energy conservation

AI Thread Summary
The discussion centers on the confusion regarding energy conservation in the context of two-slit diffraction and interference. It explains that while interference leads to an intensity pattern of 4I at bright fringes and 0 at dark fringes, the introduction of diffraction modifies this pattern, resulting in an averaged intensity lower than 2I. The key point is that energy conservation is maintained when comparing the incoming energy with the energy leaving the slits, as guaranteed by Parseval's theorem through the connection between the fields in the slit plane and observation plane. The participant grapples with intuitively understanding this conservation when diffraction is involved, suggesting that a normalization constant may be necessary to ensure energy conservation. Ultimately, the discussion highlights the complexity of reconciling interference and diffraction effects while maintaining energy conservation principles.
LmdL
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Hi all,
I have a small misunderstanding about the energy conservation in diffraction from 2 slits.
First, I understand the energy conservation of interference from 2 slits.
If intensity from each slit is I, then I have intensity of 2I after slits plane.
Interference is given by:
wJV5orO.png

So at bright fringes I get cos^2=1, so intensity is 4I. And in dark fringes I get cos^2=0, so intensity is 0.
Since interference just distributes the intensity over screen, the cos^2 pattern with 4I maximum and 0 minimum, on average, results in a 2I intensity, as just after the slits plane.
Now I add the diffraction, i.e. multiply by sinc^2. This leads to a lower intensity pattern compared to the case of pure interference, so averaged intensity will be lower then 2I. Where the energy is lost?
 
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You are comparing averages between two different situations... no special reason the averages have to be the same.
Instead, compare the incoming energy with that leaving the slits.
 
LmdL said:
Where the energy is lost?
The fields in the slit plane and in the observation plane is connected through Fourier transform in the case of far-field diffraction, therefore you don't need to worry about energy conservation because it is guaranteed by Parseval's theorem
$$
\int |E(x)|^2 dx = \int |\tilde{E}(x')|^2 dx'
$$
where ##\tilde{E}(x') = FT[E(x)]##, ##x## is coordinate in the slit plane, and ##x'## the coordinate in the observation plane.
 
Still didn't get it. I understand that this must be true (energy is conserved) and even understand why it's true (intuitive) for the interference case. But when the diffraction is introduced, I cannot get it in intuitive way. The only explanation I can think of is that I don't multiply by sinc^2 in the diffraction case, but rather by Asinc^2, where A is some normalization constant which ensures energy conservation. So the overall picture will look like that:
citPEbL.png


And not like that:
C4I1ENP.png
 
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