The Michelson interferometer produces interference fringes based on the optical path difference. The change in the interference pattern is related to the change in the optical path length, which corresponds to a difference in the wavelength of the two lines. The formula for the change in wavelength is:
\[\Delta\lambda = \frac{2 \Delta x}{m}\]
where \(\Delta x = 0.289 \, \text{mm}\) is the distance traveled by the mirror and \(m\) is the fringe order. Based on the given values, we find \(\Delta\lambda = 12 \, \text{\AA}\).
| List I | List II |
|---|---|
| A. Fraunhofer Diffraction | I. Interaction of the light waves from two different wave fronts. |
| B. Fresnel Diffraction | II. The distance between the source and the screen are effectively at infinite distance. |
| C. Interference of Light | III. It’s a phenomenon in which the wave vibrations are restricted to a particular direction in a plane. |
| D. Polarization of Light | IV. The source and screen or both are at finite distances from the aperture or obstacle. |