Buckethead said:
I think we have to accept that even a minimal universe (a universe with any amount of mass) will have to allow us to measure relative linear and relative rotational motion. If we cannot allow even that then all logic goes out the window. With this in mind I think we have to allow either of the 2 scenarios you suggest, either a universe "where motion is as motion does" or a universe where Mach's principle holds, again, regardless of how much mass is in the universe.
There's still another possibility-- if we have a universe with a kind of "minimal" mass in it, we could simply have weaker ficticious forces than in our universe, for the same acceleration. So yes, we could have relative rotation, but just a weaker centrifugal force. This of course would have to mean that inertia works differently than in Newton's laws, but that's exactly what we don't know about such "minimal" universes. It might be fun to imagine the various possible forms of Newton's laws that reduce to the familiar one in a "maximal" Machian universe, but they would be impossible to test.
If we accept the first, then if I read you correctly you are accepting an absolute frame of reference. Otherwise "motion is as motion does" does not mean anything.
It requires absolute frames only in the same way that special relativity treats inertial frames in a special way-- the frames that have no ficticious forces. I should have said "acceleration is as acceleration does", and by that I mean, the appearance of ficticious forces. In this picture, we don't say we have ficticious forces because we have an absolute acceleration, but rather we say that the presence of ficticious forces provide the
definition of absolute acceleration (that's essentially how an accelerometer works).
If a single bucket spins and it is showing concaveness, then (by definition) the bucket is spinning. And if it is spinning then it must be spinning relative to something even if that something is nothing we can define.
Right, that's the "acceleration is as acceleration does" non-Machian approach.
I do not favor this as it implies that the absolute frame of reference is moving relative to the bucket and there is no logic behind this.
Mach didn't like it much either, but it's probably the picture that has best survived general relativity, though I believe that issue is still debated among real GR experts (of which I am not one).
On the other hand if we allow Mach's principle to be described as something real formed by the motion and rotation of an object and if this "frame" is influenced by a democracy of mass then clear concise predictions about the water in the bucket can be made.
Yes, the whole approach to the "center of mass" of a system is very much a kind of "vote", as you say. It still has strange properties though-- as you say, if we have a spinning bucket with 99% of the mass of the universe, and an outside observer with 1% of the mass, the spinning bucket could "vote" that the observer is actually in orbit and the bucket is not spinning at all, and we conclude the bucket is 1% spinning and the observer is 99% orbiting. Hence we only expect a 1% bulge in the water in the bucket. Now in a universe where the observer had a million times more mass, the bulge is back to its usual scale. But the problem is, this would hold no matter how small those masses actually are, so the gravitational constant G would have to be "renormalized" based on the mass in the universe, otherwise the influences would be too small with our current G to do anything. I prefer to think of G as a fundamental constant, and only the nature of spacetime is influenced by the mass. That's why I think you need the rest of the universe to have essentially infinite mass for Mach's principle to seem reasonable, because then the gravitational influence is not negligible, it "anchors" the spacetime. Nevertheless, I could not argue that your way of renormalizing G to whatever is the total mass is impossible or wrong.
For example, if there is only a bucket of water and nothing else in the universe, then the bucket can never become concave. You can try and spin it, and it will remain flat, in other words it can never spin.
Yes, that's the fundamental question-- can a bucket spin if it is the whole universe? Mach says no, "motion is as motion does" says yes. It would be an issue of what is possible in the "initial conditions" of such a universe. Now, how would we ever know which holds true in our universe? It seems a matter of personal philosophy, as we can never do experiments in such a universe, and the testable distinctions in GR are debated even among the experts.