00:01
So in this problem, number 36, another variation of example 314 in the text.
00:08
You're a glaciologist researching the impact climate change, and you see a bubble under the surface of the ice, but you are looking at it through a groove that forms a half cylinder.
00:19
It says 86 .2 centimeters in diameter.
00:22
So that would mean the radius of that half bubble is, or that half cylinder is 43 .1 centimeters.
00:31
And optically, that would be a positive value because the bubble is to the right of the surface in my drawing, and that's a convex surface.
00:44
So the radius would be a positive number.
00:47
The image that you see through the ice appears to be at a depth of 75 centimeters.
00:55
So in this case, this is the image distance.
00:59
And it would be negative because the object is clearly under the ice as well, somewhere else, most likely over here somewhere.
01:10
But when the image and the object are on the same side of the surface, it's not really a lens in this case, but it's sort of acting as a lens.
01:20
The image distance is negative.
01:23
So we'll remember that negative sign there.
01:27
And we know it's a virtual image.
01:29
So we're going to use the equation derived in the text for a interface between curved surfaces of different indices of refraction, which is the first index of refraction divided by the object distance plus the second index of refraction divided by the image distance is equal to the difference in indices divided by the radius of that curved surface.
01:56
So we are starting from ice.
01:58
The index of refraction for ice, looking it up in the table, is 1 .309.
02:04
And then the interface goes to an index of refraction of air, which is 1.
02:11
So because we start here, we'll call this n1, and we go to air.
02:17
This is n2...