Animated Solution for Physics - Optics: A parallel beam of light is incident from air at an angle α on the side PQ of a right angled triangular prism of refractive index n=2. Light undergoes total internal reflection in the prism at the face PR when α has a minimum value of 45∘.
The angle θ of the prism is
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Visualized Solution
Analyzing the Prism
Prism PQR with angle θ at P.
Incident ray at angle α on face PQ.
Refracted ray hits face PR and undergoes TIR.
Refraction at Face PQ
By Snell’s Law at face PQ:
1⋅sinα=n⋅sinr1
Calculating r1
Given minimum α=45∘ and n=2
sin45∘=2⋅sinr1
21=2⋅sinr1
Value of r1
sinr1=21
r1=30∘
TIR at Face PR
For Total Internal Reflection at face PR:
Angle of incidence r2≥θc
Where θc is the critical angle.
Critical Angle θc
sinθc=n1=21
θc=45∘
Minimum Condition for TIR
Since α is minimum, r1 is minimum.
This makes r2 minimum.
Therefore, r2=θc=45∘
Geometry of ΔPNM
Consider the triangle formed by apex P and points M,N.
Sum of angles =180∘
∠P+∠PMN+∠PNM=180∘
Angles of ΔPNM
∠P=θ
∠PMN=90∘+r1
∠PNM=90∘−r2
Solving for θ
θ+(90∘+r1)+(90∘−r2)=180∘
θ+r1−r2=0
θ=r2−r1
Final Calculation
θ=45∘−30∘
θ=15∘
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The Sigma Insight: Refraction and Total Internal Reflection
Solution Diagram
The journey of a light ray through a prism is a beautiful interplay of Snell's Law and geometry. In this problem, we are tasked with finding the apex angle θ of a right-angled prism, given the limiting condition for Total Internal Reflection (TIR).
Analyzing the Setup
Imagine a parallel beam of light striking the vertical face PQ of a right-angled prism. The ray enters from air into the denser glass medium (with refractive index n=2) at an angle of incidence α. It bends towards the normal, traveling through the prism until it hits the second face PR. Here, it undergoes Total Internal Reflection.
Refraction at the First Face
Let's focus on the first interface, PQ. Applying Snell's Law, we can relate the angle of incidence α to the angle of refraction r1:
1⋅sinα=n⋅sinr1
We are given that the minimum value of α for TIR to occur is 45∘. Substituting α=45∘ and n=2:
sin45∘=2⋅sinr1
21=2⋅sinr1
Solving for sinr1:
sinr1=21
This tells us that the angle of refraction r1 is exactly 30∘.
The Condition for TIR
Now, let's follow the ray to the second face, PR. For TIR to happen, the angle of incidence at this face, let's call it r2, must be greater than or equal to the critical angle θc.
The critical angle is determined by the refractive index:
sinθc=n1=21
θc=45∘
Here is the crucial logical step: The problem states that α is at its minimum value. A smaller α results in a smaller r1, which geometrically leads to a smaller r2. Therefore, for the limiting case of TIR, r2 must exactly equal the critical angle.
r2=45∘
The Geometric Master Equation
To connect θ, r1, and r2, we look at the triangle ΔPNM formed by the apex P and the two points M and N where the ray intersects the prism faces.
The sum of the interior angles of this triangle must be 180∘. Let's determine these angles:
1. The top angle is simply the prism angle θ.
2. At point M, the normal is horizontal, so the interior angle is 90∘+r1.
3. At point N, the normal is perpendicular to the face PR, making the interior angle 90∘−r2.
Summing them up:
θ+(90∘+r1)+(90∘−r2)=180∘
Notice how the 90∘ terms beautifully cancel out with the 180∘, leaving us with a very elegant relation:
θ+r1−r2=0⟹θ=r2−r1
Final Calculation
We have all the pieces of the puzzle! Substitute r2=45∘ and r1=30∘ into our geometric relation: