Problem involving interference and medium with index n

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SUMMARY

The discussion centers on calculating the angular separation between the 400 nm and 600 nm lines in a first-order spectrum using a diffraction grating with 300 lines per mm, filled with water (refractive index 1.33). The participants debate the correct application of the equation for maximum localization, specifically whether to use the incident angle or the refracted angle in their calculations. The key equations discussed are d sin(θ)/n = m λ and sin(θi) = n sin(θw), with contention over the validity of each approach. Ultimately, the necessity of understanding the impact of the medium on wavelength and angle is emphasized.

PREREQUISITES
  • Understanding of diffraction grating principles
  • Familiarity with Snell's Law and refraction concepts
  • Knowledge of wavelength and refractive index relationships
  • Basic grasp of angular separation calculations in optics
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Homework Statement
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> A diffraction grating, ruled with 300 lines per mm, is illuminated with a white light source at normal incidence. (ii) Water (of refractive index 1.33) now fills the whole space between the grating and the screen? What is the angular separation, in the first-order spectrum, between the 400 nm and 600 nm lines? [5]Second the solution of the question, the equation of máximum localization is now ##d sin(\theta)/n = m \lambda##. The argument given to achieve this equation was that "the indicent plane light will suffers refraction between the two medium, such that ##sin(\theta i) = n sin (\theta w)##.

Even so i can see a logic behind this argument, i am not totally convinced with the solution of it. I mean, i am not sure of that. Honestly, i think the author is using the incident angle to measure the angular separation, and i desagree. The wave will propagate parallel to the refracted angle ##\theta w##, so the incident angle does not matter anymore. In this case, i would say that

**We could argue that the wavelength now is ##\lambda/n##. Now since the angle that matters is, in fact, the angle after the slits, already in the medium, the equation should be ##d sin(\theta w) = m \lambda /n##**.

THe problem with this solutions is that, if we substitute (Since i think both equations are essentially true, just differing the meaning of angular separation) ##\theta w## (my solution) and ##\theta i## (authors solution) in ##sin(\theta i) = n sin (\theta w)##, we did'nt got ##1=1##.

So one of the solutios is wrong. Probably mine, but i am not sure why.
 
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Herculi said:
**We could argue that the wavelength now is ##\lambda/n##. Now since the angle that matters is, in fact, the angle after the slits, already in the medium, the equation should be ##d sin(\theta w) = m \lambda /n##**.
That looks good to me.

Herculi said:
THe problem with this solutions is that, if we substitute (Since i think both equations are essentially true, just differing the meaning of angular separation) θw (my solution) and θi (authors solution) in sin(θi)=nsin(θw), we did'nt got 1=1.

I fail to see what refraction has to do with this problem.
 

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