Optics Homework: Converging Lens and Varying Refractive Index

AI Thread Summary
A rectangular slab with a linearly varying refractive index is placed in front of a converging lens, affecting the speed of light through the slab. The varying index causes different rays to travel at different speeds, resulting in a time difference as they exit the slab. This leads to the formation of a single bright spot on the screen, as the rays converge at the focal point. The problem is solved by calculating the time taken for the slowest ray to exit the slab and determining the distance traveled by the fastest ray during that time. The discussion emphasizes the optical equivalence of the slab to familiar optical devices, aiding in the understanding of light behavior.
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Homework Statement


A rectangular slab of length l=20cm and thickness d=4cm is placed in left of a converging lens of focal length f=20cm. A screen is placed in the focal plane plane of lens (right side of lens).Refractive index of the material of slab increases linearly from u0 at the bottom by an amount ##du=2*10-4)## between bottom and top faces.A parallel beam is made to incident on the left side of slab. Prove that only a bright spot forms on the screen? Find its position

Homework Equations


\Delta x=n \lambda
y=n \lambda /d

The Attempt at a Solution


Here as the refractive index varies, speed of light varies. It will be faster at bottom and slower at top.
$$v=c/ \mu$$
$$ \mu = \mu_o + y \delta \mu $$
For any two rays at y1 and y2 once the slowest ray comes out of slab,
$$t=l/v => t = l/ ( \mu_0 + d \delta \mu)$$
Hence $$ \Delta x = l(\mu_0 + d \delta \mu) \frac {(y_2-y_1) \delta \mu}{(\mu_0 + y_1 \delta \mu)(\mu_0 c + y_2 \delta \mu)} $$
 
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I'm not sure what you have calculated. What is Δx? The difference in the two path lengths?
I feel it is more useful to describe how the two light beams will be changed by the slab. Will they be bent through the same angle?
(It might help to recognise that a rectangular slab with uniformly changing index is equivalent to a more familiar piece of optics equipment.)
 
Close the thread. I have solved the problem.
 
haruspex said:
I'm not sure what you have calculated. What is Δx? The difference in the two path lengths?
I feel it is more useful to describe how the two light beams will be changed by the slab. Will they be bent through the same angle?
(It might help to recognise that a rectangular slab with uniformly changing index is equivalent to a more familiar piece of optics equipment.)
I have solved the problem. The question is of high level. Thank you for the response.
Actually \mu_1 = \mu_0 + \delta \mu
Find the time taken by slowest ray to come out of slab. Let it be t.
$$t=l \mu_1/c$$
During that time find the distance traveled by fastest ray(at bottom.
Now the situation is like fraunhoffer single slit diffraction.
 
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