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Yes. The final answer will be ## N^2 \sin^2(\frac{3 \pi}{2N}) ##.
The discussion focuses on deriving the ratio of power densities at the principal maximum and the first secondary maximum in the Fraunhofer diffraction pattern for an N-slit aperture. The key formula utilized is I=I_o \frac{\sin^2(\frac{N \phi}{2})}{\sin^2(\frac{\phi}{2})}, where \phi=\frac{2 \pi \, d \, \sin{\theta}}{\lambda}. The intensity at the primary maximum is given by I=N^2 I_o, while the intensity at the secondary maximum is calculated as I = I_0 / \sin^2(\frac{\pi}{2N}). The final ratio simplifies to N^2 \sin^2(\frac{\pi}{2N}) for large N.
PREREQUISITESStudents and professionals in optics, physicists working with wave phenomena, and anyone involved in experimental setups requiring precise measurements of light diffraction patterns.
The bottom of p.12 has the formula we used. (The ## sinc^2(\pi a u) ## is the single slit diffraction factor and is equal to 1 for narrow slits). They define ## u=\frac{\sin{\theta}}{\lambda} ## on p.3. I have seen presentations on the subject that are easier to follow. I would suggest the Optics book by Hecht and Zajac or Halliday-Resnick volume 2.says said:Will do! I've attached my notes to this comment. Pages 12-16 discuss Fraunhofer diffraction and power densities in more detail, but it doesn't have the exact equation we were using.