Diffraction Grating Vs Double-Slit: Small angle Approx.

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In double-slit interference, the small angle approximation is valid because the distance between the slits is much smaller than the distance to the screen, allowing for simplified calculations. In contrast, diffraction gratings often have slit separations comparable to the wavelength, making the small angle assumption less applicable. The intensity peaks from diffraction gratings are narrower than those from double slits, resulting in different angular distributions. While the small angle approximation can still be used for both setups at small angles, it breaks down at larger angles, highlighting a key difference in their behavior. Overall, the distinction lies in the relationship between slit spacing and wavelength, affecting the resulting interference patterns.
Beth N
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Homework Statement



In double slit interference , the angle between the center bright fringe and the path length (aka the angle used to find the path length difference) can be approximate as a small angle. However, we cannot assume the angles of bright fringes due to diffraction gratings are small. Why? What is the difference? What angles are they exactly?
Screen Shot 2018-10-27 at 9.04.54 PM.png
Screen Shot 2018-10-27 at 9.05.12 PM.png

Homework Equations



##L= tan {\theta_m}##
##dsin {\theta_m}=m\lamda##

The Attempt at a Solution


I think in double slit interference, the angle can be approximated as small because we assume the distance between the 2 slits are very small compared to the distance between the slits and the screen opposite from them. Can't see why diffraction grating is different?
 

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A hint is that it depends on the size ## d ## which is often many times the wavelength for the case of just two slits, but typically is on the order of a wavelength for the spacing of the slits or lines in a diffraction grating. That isn't always the case, but it seems to be the assumption that you need to make here. (Edit: See the 3rd paragraph below for additional comments on this). ## \\ ## An item of interest here is the intensity peaks from a multi-slit or multi-line grating are narrower in the resulting ## \Delta \theta ## than the intensity peaks from a two-slit pattern, where for a grating with many slits or lines the intensity peak can be very narrow in the angular spread ## \Delta \theta ##. You can see this in the figures above where for even 5 slits, the intensity peaks are narrower than for the two-slit case in the appearance on the screen. For the two slit case, each of the peaks is a wide blob. For the 5 slit case, the bright red region of each intensity peak is a narrower stripe. This is not why the small angle approximation can not be used for a grating though. ## \\ ## The question doesn't seem to be what I would call a very accurate question. In addition, the more important feature of the difference between the double-slit and multi-slit or multi-line grating result is the more narrow intensity peaks that result. The "small angle" approximation does still apply for both the double slit and multi-slit or multi-line grating at small angles, and starts to break down as ## \theta ## gets larger for both cases. For this reason, I think the question really misses the boat.
 
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The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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