In Part 1 of What the heck is the “speed of light?”, we noted how light in matter can move much slower than the vacuum speed of light c, or even appear to move much faster than c, under the right circumstances. We even noted that, thanks to the phenomenon of dispersion, there are cases where a single number cannot adequately describe the speed of light of a pulse in matter, because the pulse may break up into multiple pieces, each traveling at its own speed.
All of this may be summarized by saying that a pulse of light is “squishy,” and not a rigid object like a car or a softball. To measure the speed of an object, we look at how long it takes some part of the object to travel the distance from point A to point B. For a car, we can use the front bumper; for a softball, we can use its center of mass. But a pulse of light, which can change shape or break into multiple parts, there isn’t in general a clear mark we can use to define its absolute speed.
This problem of “squishiness” even arises when we look at light propagating in vacuum, and it leads to more unexpected surprises. This is what we look at in this post: the speed of light can be tricky to define sometimes, even in vacuum!
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