Max. n for TIR - air-medium interface

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The discussion centers on determining the maximum refractive index 'n' for total internal reflection (TIR) at the air-medium interface. The initial conclusion suggests that the maximum value of 'n' is √2, derived from the relationship between incident and refracted angles. However, a counter-argument indicates that there is no maximum refractive index; instead, the minimum value for 'n' that allows for TIR is √2, with 'n' being able to increase indefinitely beyond this threshold. The participants emphasize the need for mathematical rigor in the proof and clarify the implications of the critical angle in relation to TIR. Ultimately, the refractive index can be arbitrary and greater than √2, challenging the initial assumption of a maximum value.
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Homework Statement



A light ray in air is obliquely incident on a parallel-sided slab of refractive index 'n'.
The light ray refracts and hits the left side of the slab and undergoes total internal refraction.
What is the maximum possible 'n' value?

NOTE - This is a theoretical problem that I created upon observation of a numerical problem that asks for range of incident angles. I do not know if maximum 'n' value can exist for any given circumstances. Also, I have neglected the fact that at critical angle incidence, T.I.R. doesn't occur. However, a small dθ after c should cause T.I.R, so I have left out that negligible amount. Please point out any clarification and/or errors in my assumptions.

Homework Equations



n * sin θ = constant
sin c = 1 / n

The Attempt at a Solution



Now, assume the ray is incident at angle i on the top side.
Upon refraction, we can say → sin i = n * sin r.
Also, since maximum value of sin() is 1; sin i < 1 → n * sin r < 1
( we disregard i = 90°, as the ray is obliquely incident on, and not grazing, the slab)

Now, for air-slab interface, of critical angle c, we know that sin c = 1 / n.
Also, when we draw a diagram, the normals to the incident ray and refracted, T.I.R-ing ray form a right triangle, with c and r as the other two angles → c + r = 90° → c = 90° - r
Taking sin() on both sides, we get sin c = sin (90° - r) = cos r
OR, cos r = 1 / n → sin r = √(1 - ( 1 / n^2 ) ) → n * sin r = √( n^2 - 1)
OR, √( n^2 - 1) < 1 → n^2 < 2 → n < √2

Therefore, the maximum value for 'n', for ray at air-slab interface to undergo T.I.R, is √2.
 

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Bump?...
 
Your diagram is wrong angle r should be less than angle i
 
@truesearch -

My apologies! I rushed through while making the diagram on Paint.NET.

Regardless, what do you think of the proof?
 
The result is correct, but the proof is not mathematically rigorous.
So sinr≤1/n, cos(r)≤1/n...

ehild
 
What exactly does that mean?

What are the implications of this proof and your counter-arguments?

I'm a bit confused...
 
For total reflection, 90-r, the angle of incidence at the side of the slab must be greater than or equal to the critical angle θc even with the greatest r, which is equal to θc

90°-r≥θc,→ r≤90°-θc even for the greatest r:

r ≤θc≤90°-θc→ θc≤45°

The sine function is monotonously increasing between 0°and 90° so

sinθc=1/n≤1/√2 →n≥√2:

the refractive index can not be smaller than √2. √2 is the smallest, the minimum refractive index that ensures total reflection. There is no maximum refractive index. It can be arbitrary greater than √2.

ehild
 
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