csullens said:
I'm talking about the case of free-fall
I thought you were talking about a hypothetical force that is not gravity, but acts equally on all atoms in an object. If you're talking about gravity, then we already know experimentally that objects moving solely under gravity have zero acceleration--accelerometers attached to them read zero.
csullens said:
By Einstein's own thought experiment, the clocks in various places inside the elevator should all agree
If the elevator is in free fall, yes. But if the elevator is in free fall, no instruments can detect acceleration because there is no acceleration--accelerometers read zero.
You appear to be confusing two different concepts that the term "acceleration" can refer to. In GR, these concepts are called "proper acceleration" and "coordinate acceleration". Proper acceleration is the one I've been talking about, because it's the one that's directly measurable by accelerometers and is the same regardless of which coordinates you adopt. Coordinate acceleration depends on the coordinates you adopt, and in any relativistic theory no physical quantity can depend on the coordinates you adopt.
As an example of the two concepts, consider the classic apple that Newton saw falling from a tree. In coordinates in which the Earth and the tree are fixed, the apple has nonzero coordinate acceleration; but in coordinates in which the apple is fixed and the Earth and the tree are moving, the apple has zero coordinate acceleration. But in either set of coordinates, the apple has zero proper acceleration, and the Earth and the tree have nonzero proper acceleration.
csullens said:
He started by saying that there is no measurable difference between free fall in a gravitational field and floating freely in deep space right?
He did, but he also said something else: that there is no measurable difference between being
at rest in a gravitational field and
accelerating uniformly in flat spacetime. And it's the latter statement that let him figure out things about gravity. See below.
csullens said:
Then he investigated carefully the implications of such a claim. From that he deduced things about clocks changing speed
From the
second of the two statements I gave above, yes. Clocks inside a rocket accelerating in flat spacetime go at different rates--one higher up goes faster than one lower down. Einstein deduced from that that clocks inside a room at rest on the surface of the Earth would also go at different rates--one higher up goes faster than one lower down.
csullens said:
and massive bodies bending space-time,
No; the above is not enough to get to spacetime curvature. Spacetime curvature is
tidal gravity; it requires globally looking at how the "gravitational field" varies from place to place. A measure of how much harder this is than the basic insight given above is that Einstein had the basic insight given above in 1907, two years after he published SR, but it took him eight more years, until 1915, to find the correct equation--the Einstein Field Equation--that tells us how massive bodies bend spacetime.
csullens said:
it seems that the only thing that makes gravity have this property that Einstein so carefully explored, is that gravity accelerates all masses equally.
This is using "accelerates" in the sense of coordinate acceleration, which is the wrong sense. A better way to say it is the way I said it before: an object moving solely under gravity is in free fall, with zero
proper acceleration; and this is true regardless of the object's mass. In GR, this tells us that the trajectory of such a body is determined by the geometry of spacetime, not by any property of the body.
csullens said:
the only requirement for all masses to accelerate by the same amount is that the force applied is proportional to the mass
In GR, gravity is not a force. A "force" in GR is
defined as something that causes nonzero proper acceleration. The reason GR does this is that, as I said above, proper acceleration is independent of your choice of coordinates, and we want "force" in GR to also be independent of coordinates, like any physical quantity must be in a relativistic theory. (Note, btw, that this definition of "force" also applies in special relativity.)
csullens said:
it seems to me it comes back to the fact that the gravitational "charge" is mass. And the resistance to a change in inertia also mass.
This is true in Newtonian gravity, yes. But in GR, there is no such thing as "gravitational charge" in the sense you are using the term here, because, as above, gravity is not a force. And because it is not a force, "inertial mass" has nothing to do with determining the trajectory of a body moving solely under gravity either. As I said above, it's the geometry of spacetime that determines the trajectory. In other words, in GR, the "equivalence between inertial and gravitational mass" is not even a question, because there are not two separate concepts, there's only one, and it only comes into play when we subject an object to a force in the GR sense, i.e., something
other than gravity.
csullens said:
It seems to me that this is the equivalence which must be at the heart of GM.
I think you mean "GR" (General Relativity), not "GM". The equivalence which is at the heart of GR is the equivalence between a small enough patch of curved spacetime (in which gravity is present) and a small patch of flat spacetime (in which there is no gravity). This allows us to apply all the laws of special relativity in a small enough patch of spacetime even if the spacetime is curved, i.e., even if gravity is present. That means that we can learn a lot about how things work when gravity is present by applying our SR knowledge of how things work when gravity is not present. The only thing we need to add is figuring out the relationship between different small patches in a curved spacetime, i.e., in finding a global spacetime geometry that describes how all the small patches, in each of which the laws of SR apply, fit together.