haruspex said:
Every part of the scene still has straight line access to the centre of the aperture, so the light rays entering the aperture still represent the entire scene. But beyond the aperture is the lens. As the aperture is narrowed, each part of the scene can reach less of the lens and therefore contributes fewer photons to the image. Thus the brightness of the image is reduced.
True, but what matters is the light entering our eyes. While the totally, fewer number of photons would seem to come out from the image, but in reality each point on the image is still emitting the same number of photons in each direction, it's just that now they're emitting in less directions, so for an observer the brightness should remain the same. But since the aperture decreased, you could say that the field of vision is narrowed and we can see less of the image so the portion of the image that we could see would reduce, right?
haruspex said:
The refractive index, n, tells you the relative speed of light through the medium, c/n. Light travels by the shortest time route. When light passes through a medium boundary at an angle to it, the shortest time route is different from the shortest space distance; it will be biased toward spending less distance in the slower medium. When you trace the rays back to find their apparent source, you find that the apparent distance from the boundary shrinks in proportion to the refractive index of that medium. So when light travels a distance d through a medium of index n, an observer in air will perceive it has only having traveled d/n..
Yes, I know how to calculate the postion of the apparent image if you have two mediums, say a bird in
air looking at a fish in
water. The two mediums are
air and water. But in this question there are
three mediums. You have
air on the top, you have the
medium with refractive index 1.5 on top in the beaker and at the bottom of the beaker, for a depth of 40cms, you have the
medium with refractive index 1.6.
So if you were to look at the two mediums
separately, in two separate beakers, with your head in air, then you could say the
apparent depth of the bottom of the beaker = real depth/refractive index. But when you put the two mediums
together, you can't simply add the apparent depths because, for the second medium at the bottom of the beaker, light is traveling from a medium of refractive index 1.6 to one of 1.5! It's not traveling into air.
So here's what I did.
I took the bottom medium and and the upper medium and calculated the relative refractive index of the bottom medium with respect to the first. Now the actual formula if you're observing an object in a denser medium from a rarer medium that need not be air is,
apparent depth= real depth/relative refractive index of denser medium with respect to first.
So I got apparent depth if your head is in the upper medium will be
40/(1.6/1.5)
Here 40 is the real depth of the bottom of the beaker and 1.6/1.5 is the relative refractive index. So this is the apparent depth. As you move your head out into the air this virtual image can be considered as an object in the upper medium. It's depth will be,
30+(40/(1.6/1.5))
You can apply the normal formula here as you are observing from air. Then,
apparent depth= [30+(40/(1.6/1.5))]/1.5
=45
45 is the answer they got. If instead of substituting values you leave them as variables, you get the formula they used, that is,
Apparent depth for the whole thing=d1/n1+d2/n2
However, they used that without giving any explanation, so I was left confused. I still can't intuitively grasp the formula as it doesn't seem very...natural? Can anyone here get the formuala intuitively?