What Is the Angle of Incidence for Light to Emerge Parallel from a Sphere?

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The discussion focuses on calculating the angle of incidence for light to emerge parallel from a sphere with a refractive index of n=√3. The user outlines their approach using geometry, specifically an isosceles triangle formed by the light path, and applies the cosine rule and Snell's law. After deriving the angle of refraction (θ) as 30°, they use this to find the angle of incidence (i), concluding that i equals 60°. The user expresses gratitude for the assistance received, highlighting the importance of geometry in solving the problem. The thread showcases the application of mathematical principles in optics.
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[Mentor's note: this thread does not use the normal homework forum template because it was originally posted in a non-homework forum, then moved here.]

A light beam is incident on a sphere with refractive index n=√3 at an angle i from air and emerges parallel to the horizontal axis passing through the center of the sphere. Find i?

Here I made a line from the center of the sphere
25.jpg
to the exit point of the ray after which it becomes parallel to the axis. I attached a rough diagram I made in paint for it.

Now the triangle formed inside the circle is isosceles and hence two sides and corresponding angles are equal so we have two sides as r and I named the last side as d and the angle at the center is unknown. Here I only have one numerical value (n=√3) and I have to find the angle of incidence. I know there is some geometry involved so I used the cosine rule to solve for the refracted angle but even combined with snells law and other properties of triangles (S and Δ) I just don't see how to proceed, can you guys please help me out?
 
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There you go, this image should help.

note that θ=Θ-θ because it's and isosceles triangle. so Θ=2θ (θ is the angle of refraction from air to the sphere)

so √3 sin(2θ-θ) = sin(2θ)

expand the sin on the RHS you get: √3 sin(θ) = 2sin(θ)cos(θ)

solve that you get θ = 30°

now it's easy to solve this equation sin(i)=√3 sin(θ) to get i.
 

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user3 said:
note that θ=Θ-θ because it's and isosceles triangle. so Θ=2θ (θ is the angle of refraction from air to the sphere)

so √3 sin(2θ-θ) = sin(2θ)

expand the sin on the RHS you get: √3 sin(θ) = 2sin(θ)cos(θ)

solve that you get θ = 30°

now it's easy to solve this equation sin(i)=√3 sin(θ) to get i.

i=600
Thanks a gazillion. Just extending one line makes a hell of a difference, well, I guess that's geometry for you. Anyhow, thanks again. World is simpler again till I find another brainteaser from Euclid.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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