A popular pedagogical approach for introducing diffraction is to assume normal incidence of light on a single slit or a plane transmission grating. Interesting cases of diffraction from a grating at orientations other than normal incidence remain largely unexplored. In this article, we report our study of these unexplored cases, which was taken up as an undergraduate student project. We define various cases of orientation of the grating and use the Fresnel–Kirchhoff formula to arrive at the diffracted intensity distribution. An experimental arrangement consisting of a laser, a grating mount, a digital camera, and a calibrated plane screen is employed to record our observations. We discuss for each case the theoretical and experimental results and establish the conformity between the two. Finally, we analyze the details of various cases and conclude that for an arbitrary orientation of the grating, the diffraction maxima fall along a second degree curve.
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In the literature, a distinction is made between a single slit (of indefinite length, but definite width W) and a rectangular aperture (of definite length L and width W). Even though we study the rectangular aperture, we refer to it as the slit. Here, we consider a slit as a rectangular aperture with .
This arrangement of rings, which is symmetric about the middle θ ring, was arrived at by a set of repeated trials. However, determining the minimum number of inter-connected rings that can allow for all ten orientations can be an interesting group-theoretic problem.
