Find the smallest diameter of an opaque object

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Homework Help Overview

The problem involves a glass block that is 3cm thick with an index of refraction of 1.5, placed on a luminous point. The objective is to determine the smallest diameter of an opaque object that would prevent any light from escaping from the top of the block.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the implications of the luminous point's position relative to the glass block and question the clarity of the problem statement. Some explore the concept of total internal reflection and its relation to the critical angle, while others express confusion about the setup and the assumptions involved.

Discussion Status

The discussion is active, with participants offering various interpretations and questioning the assumptions made in the problem. Some guidance regarding the critical angle and total internal reflection has been provided, but there is no explicit consensus on the problem's requirements or the necessary information.

Contextual Notes

Participants note the absence of a diagram and express concern about the lack of clarity regarding the distance between the luminous point and the glass block, which may affect the interpretation of the problem.

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Homework Statement


A glass block 3cm thick and of index of refraction 1.5 is placed on a luminous point. Find the smallest diameter of an opaque object which will prevent any light from passing out of the top of the block.


Homework Equations


Snell's Law


The Attempt at a Solution



My main problem is not understanding the question. The question had no diagram attached. I assume there is no distance between the luminous point and glass block. This makes calculations difficult? However, I have checked the back of the book and there is a single correct answer.
 
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When light goes from air into a higher index material at an angle, what determines at what grazing angle you get total external reflection (no light going from air into glass)? It seems like that would be how you will get a limited cone of light in the block. Then you would project that cone up 3cm to the top surface of the glass block to figure out what the radius of the cone is there.
 
Could you perhaps explain it more clearly maybe also with a diagram? Thanks.
 
pivoxa15 said:

Homework Statement


A glass block 3cm thick and of index of refraction 1.5 is placed on a luminous point. Find the smallest diameter of an opaque object which will prevent any light from passing out of the top of the block.
As you have stated this problem, there is no opaque object that will block light passing through the top. If the luminous point is in contact with the glass block, the light will be visible at any point on the surface of the glass block.

AM
 
Andrew Mason said:
As you have stated this problem, there is no opaque object that will block light passing through the top. If the luminous point is in contact with the glass block, the light will be visible at any point on the surface of the glass block.

AM

Why? Again, a small diagram would help.
 
pivoxa15 said:
Could you perhaps explain it more clearly maybe also with a diagram? Thanks.
This site has a few diagrams that might help you: http://www.physics.louisville.edu/public/courses/phys111/davis/notes/lo_tir.html"

Andrew Mason said:
As you have stated this problem, there is no opaque object that will block light passing through the top. If the luminous point is in contact with the glass block, the light will be visible at any point on the surface of the glass block.
Why do you say that?
 
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Doc Al said:
This site has a few diagrams that might help you: http://www.physics.louisville.edu/public/courses/phys111/davis/notes/lo_tir.html"


Why do you say that?
A luminous point in contact with the block is equivalent to a light source on the block's surface emitting light in all directions (at least all directions from 0 to 180 degrees). There is no refraction or bending of the light.

AM
 
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Andrew Mason said:
A luminous point in contact with the block is equivalent to a light source on the block's surface emitting light in all directions (at least all directions from 0 to 180 degrees). There is no refraction or bending of the light.
Right... at the bottom surface of the block. But all the action (refraction, total internal reflection) takes place at the top surface.
 
Andrew Mason said:
As you have stated this problem, there is no opaque object that will block light passing through the top. If the luminous point is in contact with the glass block, the light will be visible at any point on the surface of the glass block.

AM

So you are saying the question either contains not enough information or has no right answer?

Do you think they should have specified the distance between the luminous object and the glass?
 
  • #10
berkeman said:
When light goes from air into a higher index material at an angle, what determines at what grazing angle you get total external reflection (no light going from air into glass)? It seems like that would be how you will get a limited cone of light in the block. Then you would project that cone up 3cm to the top surface of the glass block to figure out what the radius of the cone is there.

So total external reflection is light going from a lower index of refraction to a higher one. With the light reflecting off the higher index of refraction.

Since the light will only get closer to the normal after refraction, how can you get this type of reflection?
 
  • #11
pivoxa15 said:
So total external reflection is light going from a lower index of refraction to a higher one. With the light reflecting off the higher index of refraction.

Since the light will only get closer to the normal after refraction, how can you get this type of reflection?

I think Doc Al's approach is probably the correct one instead. I have a hard time dealing with the light source being right at the bottom surface, so it may be correct that the light makes it in fairly uniformly from that point. Anyways, the TIR approach probalby would limit the area more than some external reflection approach at the bottom surface anyway.

Do you understand Doc Al's hint about using TIR at the upper glass-air boundary?
 
  • #12
Ok. The question is about the critical angle for total internal reflection - the minimum angle at which all incident light is reflected back into the glass. You just have to find the radius of the circle such that light from the source strikes the upper surface at an angle that is greater than the critical angle.

The question implicitly asks you to assume that the light that is reflected from the surface back into the block does not bounce around in the glass or reflect again from the bottom so that it is able to escape through the top surface.

AM
 
  • #13
Now I finally understand the problem. All the action is indeed at the top of the surface. The light source is precisely at the bottom of the block. But the opaque object they are after should precisely be at the top of the block. At the start, I always had the impression that it was at the bottom of the block. The opaque object should block all the light coming in at an angle which is less than the critical angle. When all these refracting light it blocked, the rest will just reflect internally. So the dimension of the top surface is unimportant hence not specified which is okay. The answer came put to be 5.36cm which matches the back of the book. Thanks for the help.

Although I still don't understant how total external reflection would work (in general). Light refracting off a smaller index will bend towards the normal so how can reflection of this type occur?
 
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  • #14
pivoxa15 said:
Although I still don't understant how total external reflection would work (in general).
I assume you mean total internal reflection? Did you look at the link I provided?
Light refracting off a smaller index will bend towards the normal so how can reflection of this type occur?
Just the opposite. When light traverses a boundary from higher to lower index, the refraction is away from the normal. (A consequence of Snell's law.)
 

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