Maximum Angle of Incidence for Glass-Water Boundary?

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Homework Help Overview

The problem involves a scenario where light travels from a glass medium into a water layer, and participants are exploring the maximum angle of incidence for the light to emerge into the air above the water. The context is rooted in optics, specifically the application of Snell's Law at the glass-water boundary.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of Snell's Law and question the setup of angles in the original poster's diagram. There is a focus on understanding how angles are measured in relation to the normal and the implications of using sin(90) in the calculations.

Discussion Status

The discussion is ongoing, with participants providing feedback on the original poster's approach and questioning the assumptions made regarding angle measurement. There is an exploration of the correct interpretation of Snell's Law and its application to the problem.

Contextual Notes

Participants note potential misunderstandings regarding the definition of angles in the context of Snell's Law, particularly the distinction between angles measured from the normal versus the tangent. The original poster expresses frustration over the feedback received, indicating a desire for more substantial guidance.

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Homework Statement


A 1.0-cm-thick layer of water stands on a horizontal slab of glass. Light from a source within the glass is incident on the glass-water boundary.
What is the maximum angle of incidence for which the light ray can emerge into the air above the water?


Homework Equations


Snell's Law: nisin\thetai = ntsin\thetat


The Attempt at a Solution


I drew a diagram like this:

air (n = 1.00)
________________ light ray\uparrow
water (n = 1.33) light ray\uparrow
________________ light ray\uparrow
glass (n = 1.50) light ray\uparrow

The ray of light travels from the glass upward.

nglasssin90 = nwatersin\thetawater

nwatersin\thetawater = nairsin\thetaair

Therefore, using equality of alternate angles:

nglasssin90 = nairsin\thetaair


(1.50)*(sin90) = (1.00)*(sin\thetaair)

Solution: undefined
What is the maximum angle of incidence if it is undefined?
 
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Think about where Snell's law measures \theta from.
 
Rake-MC said:
Think about where Snell's law measures \theta from.

Sorry buddy, that was no help. After spending about an hour on that problem, I think I deserve a little more than that. I don't expect anyone to DO the work for me but come on now, let's be serious.

My question is: What is the maximum angle of incidence for which the light ray can emerge into the air above the water?
 
Yes I am aware of that, I'm showing you what you've done wrong.
For a ray of light perpendicular to the surface, you wrote: n_1sin(90)
Why did you write sin(90)?
Think of where snell's law measures \theta from.
 
Rake-MC said:
Yes I am aware of that, I'm showing you what you've done wrong.
For a ray of light perpendicular to the surface, you wrote: n_1sin(90)
Why did you write sin(90)?
Think of where snell's law measures \theta from.

If it is incident it's perpendicular and if it's perpendicular it's 90 degrees.
 
90 degrees from the tangent.
doesn't Snell's law measure \theta from the normal?
 
Rake-MC said:
90 degrees from the tangent.
doesn't Snell's law measure \theta from the normal?

Ok, so that makes it 45 degrees?
 

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