Atmospheric optics
Last night I stepped outside around 23:00. There were some high, thin, even clouds and a full moon almost directly overhead. Together, they made for a stunningly clear lunar corona plus a 22º halo. The halo was very tight and the corona was amazingly well-defined, with a very distinct spectrum as it faded off at the edges. Marvelous.
But also very interesting. Atmospheric optics give wonderful insight into the field of optics in general, where light is modelled with either rays, bending as it passes from one medium to another and propagating in straight lines apart from that, or waves, spreading out like ripples in a pond. Each optical effect comes from a specific sort of atmospheric condition. My descriptions here are adapted from the site linked above, which also has pictures illustrating what I’m talking about.
The 22º halo is created by relatively large crystals of ice suspended in the air, which are shaped like hexagonal prisms. It occurs when rays of light from the moon hit these crystals of ice, which act as little prisms. If a ray of light hits one side of the hexagon it bends before passing through the crystal. When it hits another face it bends again as it leaves the crystal. If the entering and exiting faces are at 60º to each other, the total bending will be between 22º and 50º, mostly at the lower end of this region. Since the moon is so far away that we can approximate all the rays coming in parallel the crystals that bend light rays 22º and then send them on to our eyes will all lie on a cone with cone angle 22º. When we see thos crystals lit up, that’s the halo.
The corona, on the other hand, arises as a diffraction effect. Tiny particles, like water droplets or very small ice crystals in a cloud, behave like pebbles in the path of the onrushing light wave. Instead of an even, parallel wavefront, each point on the particle’s surface scatters a new wave starting at that point. As all these new waves rush over each other, parts of them reinforce and parts cancel out. The pattern of such “interference fringes” is familiar from the usual explanation of the quantum-mechanical “double-slit” experiment, which is another diffraction effect. Further, since the color of light influences the length of its waves the peaks of intensity for different colors will be in different places. Near the moon itself the fringes stack up and the whole cloud is illuminated, but out towards the edge the red fringes are further apart than the blue fringes, which leads to the spectrum effect at the corona’s edge.
It’s amazing that just by looking up at the right time I could see evidence of exactly what was going on in the sky above me. The clouds consisted of ice crystals in a somewhat heterogenous mixture. Smaller crystals directly overhead diffracted the moon’s light into the corona, while larger crystals refracted the light to form the halo.
The two effects also relied on two different properties of light. The halo comes from treating light as little particles flying along straight lines, while the corona depends on treating light as a wave. That means that the display wouldn’t have been possible without quantum mechanics!
I’ve said it before and I’ll probably say it again: Science. It works.
