Fraunhofer diffraction integra theorem

In summary, the Electric Field complex amplitude at a point P can be computed by an integral that is applied to the sum of all the point surface elements of a given aperture, even if the aperture is composed of line surface elements.
  • #1
pop_ianosd
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2

Homework Statement


This is not an actual problem, it is a general matter about the equation that describes the Fraunhofer diffraction;
So, for a given aperture(A), which is evenly illuminated from the left(let's say), the Electric Field complex amplitude at a point P(on the right-the screen) can be computed by the formula:

E[itex]_{P}[/itex] = K[itex]\int[/itex][itex]_{A}[/itex]e[itex]^{ikr}[/itex]dA,
where r is the distance from the surface element dA to the point P.

My questions concerns the fact that I have seen this integral being applied (in a physics book) to non-point surface elements dA, but to line surface elements(dA = Ldy).
The problem I see about this is that one cannot define a distance r between a point and a line-surface element.
The exact case was at calculating the diffraction pattern given by a rectangular (Width>>Height) aperture, and later for a circular aperture.
How is this possible?


Homework Equations





The Attempt at a Solution

 
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  • #2
I think we can consider the line surface element as a collection of point surface elements, each one with its own corresponding distance. The integral is then applied to the sum of all the point surface elements, which results in some way in the same integral being applied to the line-surface element. This means that the integral should not be applied directly to the line surface element, but rather it should be applied to the sum of all the point surface elements that are part of it.
 

1. What is the Fraunhofer diffraction integral theorem?

The Fraunhofer diffraction integral theorem is a mathematical formula that describes the diffraction of light waves by an aperture or object. It is used in optics and physics to calculate the intensity and distribution of light after it passes through an aperture or diffracting object.

2. How is the Fraunhofer diffraction integral theorem derived?

The Fraunhofer diffraction integral theorem is derived from the Huygens-Fresnel principle, which states that each point on a wavefront can be considered as a source of secondary spherical waves. These secondary waves then interfere to produce the overall diffraction pattern. By analyzing the interference of these secondary waves, the Fraunhofer diffraction integral theorem is derived.

3. What is the difference between Fraunhofer and Fresnel diffraction?

The main difference between Fraunhofer and Fresnel diffraction is the distance between the aperture or diffracting object and the screen where the diffraction pattern is observed. In Fraunhofer diffraction, the distance is large compared to the size of the aperture, while in Fresnel diffraction, the distance is comparable to the aperture size. This results in different mathematical treatments and different diffraction patterns.

4. What are some real-life applications of the Fraunhofer diffraction integral theorem?

The Fraunhofer diffraction integral theorem has various applications in optics and photonics, such as in the design and analysis of optical devices like lenses, mirrors, and diffraction gratings. It is also used in the study of diffraction phenomena in crystal structures, as well as in medical imaging techniques like X-ray diffraction and electron diffraction.

5. Are there any limitations to the Fraunhofer diffraction integral theorem?

Yes, the Fraunhofer diffraction integral theorem has some limitations. It assumes that the diffracting object is thin and has a smooth surface, and that the light source is monochromatic. It also does not take into account the effects of polarization and scattering. In some cases, these assumptions may not hold true, and the diffraction pattern may deviate from the predicted results.

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