Diffraction from a single slit, with Lens

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Homework Help Overview

The problem involves diffraction from a single slit with a lens, specifically analyzing the behavior of light passing through a slit and focusing through a lens to determine the slit width based on given parameters such as wavelength and distances in the focal plane.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the relationship between the angles of incident and emerging rays, the derivation of fringe spacing, and the implications of the lens on the diffraction pattern. There are attempts to clarify the use of focal length in calculations and the effects of the lens on the light rays.

Discussion Status

The discussion is ongoing with various interpretations being explored. Some participants have offered insights into the derivation of equations relevant to the problem, while others question the assumptions regarding the lens's effect on the diffraction pattern.

Contextual Notes

Participants note the specific setup of the problem, including the placement of the slit on the lens and the significance of the focal length in relation to the distance to the screen. There is also mention of the need to consider the refraction effects of the lens in the calculations.

JosephK
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Homework Statement


Parallel rays of green mercury light with a wavelength of 546 nm pass through a slit covering a lens with a focal length of 60.0 cm. In the focal plane of the lens the distance from the central maximum to the first minimum is 10.2 mm. What is the width of the slit


Homework Equations



a/2 sin theta = lambda / 2


The Attempt at a Solution



Tangent theta is opposite over adjacent... The adjacent, I think, is the focal length, 60.0 cm. The opposite is clearly 10.2 mm. So, tan theta = 10.2 mm / 600 mm. Then to get a, the width of the slit, I use the above equation.

I am not familiar with lenses. So, I am not sure if the "adjacent" is correct.
 
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Hmmm ... without the lens, dsinθ=nλ and Ltanθ=Δx: L is the distance to the screen and d is the separation of the slits.

In the limit L >>d, what happens to these equations?

The effect of the slits is to produce maxima "rays" that are diverging: they fan out.
The effect of the lens is, presumably, to converge the rays - so they fan out less.
Your calculation would be for the same situation without the lens.

So you need to be able to relate the angle of the ray incident to the lens with the angle of the emerging ray.
 
I have just tried this question and I believe I have the answer - not sure if you have by now, but for any others out there...

The trick is to realize how to derive the formula for the fringe spacing of minima produced by the single slit.
y = m\lambda L / a
In that derivation, L was used as the distance to the screen- With a lens: L must be equivalent to the focal length, f. So that y = fringe spacing = (m\lambda f)/a . Where a is equal to the slit width, \lambda : wavelength of light.
Hope that's right! Good luck all!
 
@elette:
Welcome to PF;
In this problem the slit is right on the lens and the screen is in the focal plane - so L=f ... fine.
Thinking of the derivation of the fringe-spacing equation is important - however:
In that derivation, L was used as the distance to the screen- With a lens: L must be equivalent to the focal length, f. So that y = fringe spacing = (m\lambda f)/a . Where a is equal to the slit width, \lambda : wavelength of light.
... $$\Delta y = \frac{\lambda f}{a}$$ ... does not appear to account for the refraction of the light through the lens.
Does the lens have no effect at all?
 

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