AcademyDiffraction

Academy

Fresnel and Fraunhofer Regimes

Level 1 - Physics topic page in Diffraction.

Principle

Diffraction is wave spreading caused by a finite aperture or obstacle. The observed pattern depends on wavelength, aperture size, and distance from the aperture.

Fresnel diffraction is near-field diffraction, where wavefront curvature still matters. Fraunhofer diffraction is far-field diffraction, where the pattern depends mainly on angle.

Notation

\(a\)
aperture or slit width
\(\mathrm{m}\)
\(L\)
distance from aperture to screen
\(\mathrm{m}\)
\(\lambda\)
wavelength
\(\mathrm{m}\)
\(N_F\)
Fresnel number
1
\(\theta\)
observation angle
\(\mathrm{rad}\)

Method

Derivation 1: Use Huygens wavelets

Each point across an aperture acts as a source of secondary wavelets. The final pattern is set by the phase relationships between those wavelets.

Wavelet phase difference
\[\Delta\phi=\frac{2\pi\Delta r}{\lambda}\]
Far-field path difference across width
\[\Delta r\approx a\sin\theta\]

Derivation 2: Classify the regime

The Fresnel number compares aperture size with diffraction spreading over distance \(L\).

Fresnel number
\[N_F=\frac{a^2}{\lambda L}\]
Fraunhofer tendency
\[N_F\ll1\]
Fresnel tendency
\[N_F\gtrsim1\]

Derivation 3: Relate angle to screen position

In the far field, positions on a distant screen correspond directly to diffraction angles.

Screen geometry
\[y=L\tan\theta\]
Small-angle form
\[y\approx L\theta\]

Rules

Fresnel number
\[N_F=\frac{a^2}{\lambda L}\]
Far-field path difference
\[\Delta r\approx a\sin\theta\]
Small-angle screen position
\[y\approx L\theta\]

Examples

Question
A slit has
\[a=0.20\,\mathrm{mm}\]
\[L=2.0\,\mathrm{m}\]
and
\[\lambda=500\,\mathrm{nm}\]
Estimate \(N_F\).
Answer
\[N_F=\frac{(0.20\times10^{-3})^2}{(500\times10^{-9})(2.0)}=0.040\]
This is in the Fraunhofer range.

Checks

  • Diffraction becomes important when an aperture dimension is comparable with the wavelength.
  • Fraunhofer patterns are usually simpler because they are angular patterns.
  • Increasing \(L\) lowers \(N_F\), pushing the setup toward the far field.
  • The small-angle screen formula needs \(y\\ll L\).