sol invictus
Philosopher
- Joined
- Oct 21, 2007
- Messages
- 8,613
I strongly suspect that there's a force on the tapered walls of the cavity that balances out the difference exactly, but I'd have to revise a lot of stuff I haven't looked at for a quarter of a century before I could work it out.
It depends a little on what the initial state of the of the microwaves is.
Think of some marbles in a can in space (make the can tapered if you want, or any shape). You can imagine a configuration where the can is at rest, but all the marbles are flying towards one end. When they hit, they'll scatter in many directions, and the thing will settle down to a state where the whole can moves in the direction the marbles were originally going (since the average momentum carried by the marbles themselves after they have time to scatter a few times will be close to zero).
(You could do this experiment - take a basin of water, shake it once to make a wave, and quickly set it down on ice or some other slippery surface before the wave hits the side. The whole thing will slide off, jolting a little as the waves settle down.)
Contrast that with the case where the can is at rest and the marbles are flying around randomly. It's obvious that no matter what the shape of the can is, it will never start accelerating off in some direction (or even move much except for some little vibrations from bouncing marbles).
So you could probably arrange a configuration of EM fields that would give the thing a little kick at the beginning, but only because you started off with that momentum. You can't change the net momentum so long as nothing leaves the can, and the shape is totally irrelevant to that. So yes, there's a force on the tapered sides exactly that cancels the one he computed. No work necessary.
Last edited: