Fizeau’s Fringes
Fizeau’s fringes are fringes of equal thickness produced by the interference of light reflected from the two surfaces of a thin wedge-shaped film.
- They are generally straight, parallel, and equally spaced.
- They are localized near the film.
- The thickness of the film varies from point to point.
- The optical path difference depends on the thickness of the film.
For a film of refractive index μ, thickness t, and refracted angle r:
Δ = 2μt cos r
For a wedge-shaped air film at nearly normal incidence:
Δ = 2t
The condition for dark fringes in reflected light is:
2t = mλ
If the wedge angle is θ, then:
t = xθ
Therefore:
2xθ = mλ
The fringe width is:
β = λ / (2θ)
Difference Between Haidinger’s and Fizeau’s Fringes
| Property | Haidinger’s Fringes | Fizeau’s Fringes |
|---|---|---|
| Type | Fringes of equal inclination | Fringes of equal thickness |
| Film | Plane-parallel film | Wedge-shaped film |
| Shape | Circular | Circular, Straight and parallel |
| Localization | At infinity | Near the film |
| Main variable | Angle of inclination | Film thickness |
| Typical example | Plane-parallel plate | Air wedge |
| Fringe spacing | Generally not uniform | Uniform for a uniform wedge |