Validity of Fresnel Approximation

In summary, the Fresnel diffraction approximation is valid when the Fresnel number is approximately 1. This condition is dependent on the maximum angle involved and the validation condition for the approximation is when a is much smaller than the relation between 4z^3 and lambda. In the near radiation zone, we see a parallel beam with a waist and possible hot spots, while in the far radiation zone, the beam diverges at an angle defined by the aperture size and may have sidelobes. This is different from the reactive near field, which occurs at fractions of a wavelength from a source.
  • #1
yucheng
232
57
Wikipedia says that Fresnel diffraction is valid if the Fresnel number is approximately 1. What Fresnel number then is the Fresnel approximation for paraxial-paraboloidal waves valid? It's not mentioned...

Oh I just realized that

$$\frac{N_F \theta_m^2}{4} \ll 1$$

So it depends on the maximum angle... Oops

Anyway, we have the validity condition for Fresnel Approximation ##a^4 \ll 4 z^3 \lambda##

So.. for what a is it valid? How small should ##a## be given the relation ##\ll##, that is rather arbitrary?

Suppose ##z = 1 m##, ##\lambda = 633 \\ nm## (Exercise 2.2-1, Fundamentals of Photonics, Saleh & Teich)

Thanks in advance!
 
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  • #2
My simple understanding as a microwave engineer is that for the case of waves emerging from an aperture, if we are close to the aperture we have Fresnel conditions and if we are far we have Fraunhofer conditions. The two regions are sometimes referred to as the near and far radiation zones. The boundary is ill defined, and occurs at the Rayleigh Distance, which may be defined as (Diameter^2) / 2 lambda. In the Fresnel region we tend to see a parallel beam, but it usually has a waist and can also have hot spots. Maybe it can also have a black dot in the middle. In the Fraunhofer region the beam diverges at an angle defined by the aperture size in wavelengths, and we also see sidelobes, which are mainly defined by the illumination taper of the aperture. The radiation pattern in the Fraunhofer region does not change with distance.
The near radiation zone is not to be confused with the reactive near field, which occurs at fractions of a wavelength from a source, so we need care in using the terminology.
 
  • #3
I like Fresnel is "intermediate far" and Fraunhofer is "far". But of course the near and far radiation zone is a better description.
 

1. What is the Fresnel Approximation?

The Fresnel Approximation is a mathematical method used to approximate the diffraction pattern of a wave passing through a small aperture or around an obstacle. It is based on the assumption that the aperture or obstacle is small compared to the wavelength of the wave.

2. How is the validity of the Fresnel Approximation determined?

The validity of the Fresnel Approximation is determined by comparing the results obtained using the approximation with the exact solution of the diffraction problem. If the results are similar, then the approximation is considered valid.

3. What are the limitations of the Fresnel Approximation?

The Fresnel Approximation is only valid for small apertures or obstacles and for waves with a long wavelength compared to the size of the aperture or obstacle. It also does not take into account the effects of edge diffraction and multiple scattering, which can significantly affect the diffraction pattern.

4. How does the Fresnel Approximation differ from the Fraunhofer Diffraction?

The Fresnel Approximation is a more general method that can be applied to a wider range of diffraction problems, while the Fraunhofer Diffraction is a specific case of the Fresnel Approximation for an infinitely distant screen. The Fresnel Approximation also takes into account the curvature of the wavefront, while the Fraunhofer Diffraction assumes a flat wavefront.

5. Can the Fresnel Approximation be used for all types of waves?

The Fresnel Approximation can be used for any type of wave, as long as the wavelength is much larger than the size of the aperture or obstacle. This includes electromagnetic waves, such as light and radio waves, as well as sound waves and water waves.

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