Understanding Dark Fringe at Contact Lenses

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SUMMARY

The discussion focuses on the phenomenon of dark fringe formation at the center of contact lenses due to interference effects. It explains that the path difference between rays reflected from the top and bottom of the air gap at the lens contact point is zero, but the ray from the denser medium experiences a 180-degree phase shift. This results in a dark spot at the center, as the condition for maxima indicates that the nearest maxima occurs at a radius greater than zero, confirming that the center is dark.

PREREQUISITES
  • Understanding of optical interference principles
  • Familiarity with phase shifts in wave optics
  • Knowledge of plano-convex lens geometry
  • Basic mathematical skills for applying binomial expansion
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  • Study the principles of optical interference in detail
  • Learn about phase changes in reflection and transmission
  • Explore the mathematics of circular interference patterns
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Homework Statement



I'm unable to understand the production of dark fringe in the central point of contact of lens.The text says "the path difference between the rays reflected at the top & bottom of air gap at the point of contact is zero.Actually the ray reflected from the top of air film doesn't undergo any change in phase but the ray reflected from bottom of air film i.e denser medium suffers a phase change of 180 degrees or additional P.D of lambda/2.Hence dark spot is formed".Plz. explain in simple words.Thanks.

Homework Equations


Nill.

The Attempt at a Solution

 
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Suppose the radius of curvature of the lens(plano-convex, I studied that before, couldn't quite remember) = R, and the incident light is directed towards the lens upright.

We're now concerned with the radii of circular inteference,r.

As you've said, we're concerned with the phase change(180) caused by the reflection at the denser medium UNDER the air film.

So, the condition for maxima is given by 2d = (m + 1/2)lambda for m = 0,1,2,..

We now find the relationship of d, thickness of air film, corresponding to the distance,r away from the center of the lens.

d = R - (R^2 - r^2)^1/2
= R - R[1 - (r/R)^2]^1/2

by binomial expansion, d approximates to (r^2)/2R

Put it in d = (m+ 1/2)lambda,
r = [(m+1/2)*lambda*R]^1/2 for m = 0,1,2,...

That means, for m = 0, r must be something larger than 0, and we're talking about maxima now. Simply put, for m = 0, the nearest maxima is not on the center where r = 0 because we've calculated that r>0.

Thus, center should be dark.
 

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