WHY IS THE SKY BLUE?

WAVELENGTH AND DISCRIMINATION

If waves are made at the side of a lake and a rock is sticking out of the water, a little off shore, when they reach it, do the ripples "see" the rock - do they bounce off it, bend round it - or do they pass it by, as if nothing was there? If the wavelength of the waves (the distance between crests) is smaller than, or equal too (roughly) the size of the rock, the waves "see" it. If they are longer than the rock they pass by unchanged. For this reason a light microscope may only discriminate detail of a size equal to the wavelength of light. Finer detail requires an electron microscope - electrons have a shorter wavelength than photons because of their high momentum. (See: Quantum Mechanics Basic Idea.) White light contains blue wavelengths. If there are the appropriate sized "rocks" in the air the problem is close to being solved.

SUNLIGHT JUST MISSING THE EARTH

If a searchlight beam was looked at from the side nothing would be seen, unless there was some sideways scatter of the light. Some light from the Sun just misses the Earth. If it were not scattered (some of it downward) by the atmosphere none of it would ever illuminate the surface. If the blue light is scattered - if there is something in the atmosphere blue waves can "see" - then, when someone looks up at the sky, they will observe blue.

The problem is there are no particles in the atmosphere of the appropriate size.

ATMOSPHERE PARTICLES

All molecules and atomic scale particles are too small. Neither are the various dust particles appropriately sized; they would scatter all wavelengths, not pick out the blue. Indeed, if a glass tube is filled with perfectly dustless, clean air and white light shone along it, blue light scatters out of the sides. It is clear therefore that it is the air itself and not any sophistications which is responsible for dissipating blue light.

RESOLUTION OF THE "PARADOX," HOLES IN THE SKY

There is no particle in the atmosphere of an appropriate size to scatter blue light; we appear to be up against a brick wall.

The - rather elegant, perhaps - resolution of this metaphorical paradox is gained by imagining the air to consist in many particles flying about at random. By pure chance there will exist holes in the air where, simply by chance, no particles happen to be. These holes are the desired size, turning the sky blue.

PREDICTION

Should the Earth's covering of gas get thinner, for any reason, it is easy to see that the holes in the sky would grow larger and the sky would turn red.

SHEPHERD'S DELIGHT

The Sun is red when low in the sky because its light has traveled through a large thickness of atmosphere, before reaching the eye and the scattering of the blue sideways, throughout its journey, has left only the longer, redder wavelengths.

SHEPHERD'S WARNING

Bugger off or I'll shove a sheep up your tradesman's entrance.


[Note of caution: This frequently asked question was addressed in New Scientist magazine; the above explanation was not among those printed.]

Quote from Kung 'No offence Sporus but the reason it wasn't printed is probably because it's piffle.' This raises an interesting point. I got the theory from a book by Jeans. Jeans and Rayleigh worked together (recall the Jeans-Rayleigh Law). Perhaps they fell out over the sky blue question. I'd back Jeans, he was unquestionably a genius.