Since you are interested in the proof via Snell's law, I should specify that you can use the small angle approximation in this case. Do you know how to do this for a single layer of material, like finding the apparent depth of a coin at the bottom of a pool?
rno88 said:
The ray that merges into the benzene from the air is refracted toward the normal because n of benzene > n of air.
Yep.
rno88 said:
Then as that ray merges into the water is is refracted toward the normal because n of benzene > n of water.
Nope. You got it backwards. I'm assuming you are tracing the ray from the benzene into the water.
rno88 said:
The path of the ray we see is imaginary ...
I don't know what you mean by that. The depth that your brain reconstructs from the rays that enter your eye is imaginary in that, if you plunge a ruler into the container down to that depth, you will not hit the bottom, because it isn't the true depth. So, the point in space where your brain thinks that the rays intersect is not where they actually do. However, the rays that finally enter your eye after being refracted and reflected by whatever means are always real in any situation.
rno88 said:
... is there one set of ... rays that got through both the benzene and the water?
Yes. I assume you mean that, for each physical ray in the set, you can trace it along a unique path from a point on the bottom to a point at the surface of the benzene.
rno88 said:
... how do you find the ray paths with only knowing the depth? It seems that there is not enough information to use Snell's.
You can just choose a point on the bottom and consider the paths of two different rays that originate from that point out into the air. Draw a picture with three horizontal lines: the bottom line represents the bottom, the middle line represents that water-benzene boundary, and the top represents the surface of the benzene. Then, choose a point on the bottom line and draw from it two
almost vertical lines, but slightly slanted. When these lines intersect the middle horizontal line, they become more vertical (they bend toward the normal from the water to the benzene). Continue these new segments until they hit the top horizontal line. At that point, the lines become more slanted (even more so than in the bottom layer, because n_air<n_water).
You can write equations for the rays in the air, for instance in slope-intercept form, and then solve for the intersection of these two lines.