Amplifies? The Schwarzschild spacetime (which behaves like Newtonian gravitational field in large distance limit) needs only one point-like massive object. What do you expect as a non-negligible difference made by (non-)existence of distant objects?
What do you expect as a non-negligible difference made by (non-)existence of distant objects?
The fact that there’s no longer a frame against which to measure local rotation in any sense other than its rotation relative to the frame of the other body. So it makes a big difference what counts as “the rest of the universe”.
People believed for a quite long period of time that the distant stars don’t provide a stable reference frame. That it is the Earth which rotates was shown by Foucault pendulum or similar experiments, without refering to outer stellar frame.
(two points, one about your invocation of frame-dragging upstream, one elaborating on prase’s question...)
point 1: I’ve never studied the kinds of tensor math that I’d need to use the usual relativistic equations; I only know the special relativistic equations and the symmetry considerations which constrain the general relativistic equations. But it seems to me that special relativity plus symmetry suffice to justify my claim that any reasonable mechanical apparatus you can build for reasonable-sized planets in your example will be practically indistinguishable from Newtonian predictions.
It also seems to me that your cited reference to wikipedia “frame-dragging” supports my claim. E.g., I quote: “Lense and Thirring predicted that the rotation of an object would alter space and time, dragging a nearby object out of position compared with the predictions of Newtonian physics. The predicted effect is small—about one part in a few trillion. To detect it, it is necessary to examine a very massive object, or build an instrument that is very sensitive.”
You seem to be invoking the authority of standard GR to justify an informal paraphrase of version of Mach’s principle (which has its own wikipedia article). I don’t know GR well enough to be absolutely sure, but I’m about 90% sure that by doing so you misrepresent GR as badly as one misrepresents thermodynamics by invoking its authority to justify the informal entropy/order/whatever paraphrases in Rifkin’s Entropy or in various creationists’ arguments of the form “evolution is impossible because the second law of thermo prevents order from increase spontaneously.”
point 2: I’ll elaborate on prase’s “What do you expect as a non-negligible difference made by (non-)existence of distant objects?” IIRC there was an old (monastic?) thought experiment critique of Aristotelian “heavy bodies fall faster:” what happens when you attach an exceedingly thin thread between two cannonballs before dropping them? Similarly, what happens to rotational physics of two bodies alone in the universe when you add a single neutrino very far away? Does the tiny perturbation cause the two cannonballs discontinously to have doubly-heavy-object falling dynamics, or the rotation of the system to discontinously become detectable?
Amplifies? The Schwarzschild spacetime (which behaves like Newtonian gravitational field in large distance limit) needs only one point-like massive object. What do you expect as a non-negligible difference made by (non-)existence of distant objects?
The fact that there’s no longer a frame against which to measure local rotation in any sense other than its rotation relative to the frame of the other body. So it makes a big difference what counts as “the rest of the universe”.
People believed for a quite long period of time that the distant stars don’t provide a stable reference frame. That it is the Earth which rotates was shown by Foucault pendulum or similar experiments, without refering to outer stellar frame.
(two points, one about your invocation of frame-dragging upstream, one elaborating on prase’s question...)
point 1: I’ve never studied the kinds of tensor math that I’d need to use the usual relativistic equations; I only know the special relativistic equations and the symmetry considerations which constrain the general relativistic equations. But it seems to me that special relativity plus symmetry suffice to justify my claim that any reasonable mechanical apparatus you can build for reasonable-sized planets in your example will be practically indistinguishable from Newtonian predictions.
It also seems to me that your cited reference to wikipedia “frame-dragging” supports my claim. E.g., I quote: “Lense and Thirring predicted that the rotation of an object would alter space and time, dragging a nearby object out of position compared with the predictions of Newtonian physics. The predicted effect is small—about one part in a few trillion. To detect it, it is necessary to examine a very massive object, or build an instrument that is very sensitive.”
You seem to be invoking the authority of standard GR to justify an informal paraphrase of version of Mach’s principle (which has its own wikipedia article). I don’t know GR well enough to be absolutely sure, but I’m about 90% sure that by doing so you misrepresent GR as badly as one misrepresents thermodynamics by invoking its authority to justify the informal entropy/order/whatever paraphrases in Rifkin’s Entropy or in various creationists’ arguments of the form “evolution is impossible because the second law of thermo prevents order from increase spontaneously.”
point 2: I’ll elaborate on prase’s “What do you expect as a non-negligible difference made by (non-)existence of distant objects?” IIRC there was an old (monastic?) thought experiment critique of Aristotelian “heavy bodies fall faster:” what happens when you attach an exceedingly thin thread between two cannonballs before dropping them? Similarly, what happens to rotational physics of two bodies alone in the universe when you add a single neutrino very far away? Does the tiny perturbation cause the two cannonballs discontinously to have doubly-heavy-object falling dynamics, or the rotation of the system to discontinously become detectable?