Double Slit Diffraction with Angled Light

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Homework Help Overview

The discussion revolves around a double slit diffraction problem involving interference maxima and the relationship between angles and distances. The original poster is attempting to solve for the position of the interference maxima, denoted as ym, while navigating the complexities of angle θ and the fixed angle β.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster sets up equations for sinθ and tanθ to relate them to the position of maxima. They express confusion about the fixed angle and the relevance of β. Other participants suggest using geometric considerations to analyze the paths of light and clarify the conditions for maxima.

Discussion Status

Participants are exploring various approaches to relate the angles and distances involved in the diffraction problem. Some guidance has been offered regarding the geometric interpretation of the paths, but there remains uncertainty about the assumptions being made, particularly concerning the fixed angle β and how to express θm in terms of other parameters.

Contextual Notes

There is mention of a small-angle approximation and the need for specific values such as wavelength and slit separation, which are not provided. The discussion reflects the complexities of the problem setup and the assumptions that may influence the approach taken.

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Homework Statement
Suppose that a laser beam hits a double-slit apparatus at an angle of β = 40 degrees with respect to the normal. The screen is a distance L away, with slit width a and slit separation d.

Derive a symbolic expression for locating the double-slit interference maxima. At what angle θo is the center of the interference pattern located on the screen? Is the interference pattern symmetric about that angle?
Relevant Equations
dsinθ = mλ (maxima)
tanθ = ym / L
Given that [y][/m] is equal to the position of the interference maxima and is the variable I’m solving for. I got as far as setting up two expressions, one for sinθ and the other for tanθ.

sinθ = (mλ)/d
tanθ = ym/L

My first instinct was to set θ = 40 degrees. By relating sinθ and tanθ to each other through cosθ, I get:

ym = (Lmλ) / (dcos40)

However, I don’t think this makes sense if I have to solve for θo in the second part of the question, so θ must not be fixed. I’m confused about how I am supposed to use the given value of β, but I assume it must be relevant.

If I were able to use small-angle approximation, sinθ ≈ tanθ, but does this still apply here?
 

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There are many ways to do this. Personally I would look at the two paths and figure the difference in distance using plane geometry. ( Make a good drawing of the path near the plate. ) Then write down the condition for each max assuming β to be held fixed
 
This drawing is from my notes, but this is also what I was thinking for this problem. (Ignore the s1, that’s just a reference point.) I‘m still a bit confused by what you mean with “the condition for each max assuming β to be held fixed.” In this case, β is explicitly held fixed at 40 degrees, no? Is there an assumption I’m making without realizing it?
 

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Yes I meant that you are interested in solving for θm (in fact only for θ0 ) in terms of the other parameters.
 
I see what you mean and why that is the goal, but I‘m still short-circuiting on what to do in order to get there. For instance, I suppose I could say θm = sin-1[(mλ)/d] = tan-1(ym/L), but is that really a sufficient symbolic expression?

And assuming that it is, how does that help me find θo since I don’t know wavelength or slit separation?
 

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