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Do you have an example? I can imagine a gravitational field generated by an infinite plane. In that case the field is uniform and there are no tidal forces. But infinite planes were not detected by astronomers until now.
If there are tidal forces, and the Riemann tensor is not zero, some Christoffel symbols must be non zero.
What according to the Einstein text (..non-vanishing of the components of the affine connection...) => gravitational field.
Quote from: saspinski on 22/04/2018 22:39:27Quote from: PmbPhy on 21/04/2018 17:20:24You did get lost. Its not possible to have a non-zero Riemann tensor for a uniform gravitational field. Its actually the definition of a uniform field.Yes, I changed a γ by a δ of one of the Γ's. There are a lot of them. But now I checked everyone, and all components are really zero. So, in the specific case of an uniform gravitational field, the spacetime is flat for any observer (being or not in free fall).For conventional (non uniform) gravitational fields, the spacetime is curved for any observer. The gravitational field of a vacuum domain wall has zero curvature everywhere off the wall itself. In this case the wall is repulsive. The field around a straight cosmic string is zero for both the curvature and there is no gravitational field around the string giving the space around it a conical solace but does not exert gravitational forces on things nearby.
Quote from: PmbPhy on 21/04/2018 17:20:24You did get lost. Its not possible to have a non-zero Riemann tensor for a uniform gravitational field. Its actually the definition of a uniform field.Yes, I changed a γ by a δ of one of the Γ's. There are a lot of them. But now I checked everyone, and all components are really zero. So, in the specific case of an uniform gravitational field, the spacetime is flat for any observer (being or not in free fall).For conventional (non uniform) gravitational fields, the spacetime is curved for any observer.
You did get lost. Its not possible to have a non-zero Riemann tensor for a uniform gravitational field. Its actually the definition of a uniform field.
Ok, I still don't understand why gravity exists though. Why do two masses attract?
I reckon that the gravitational field around an infinitely long straight wire (or a long straight string) is not zero –
Quote from: Mad Aetherist I reckon that the gravitational field around an infinitely long straight wire (or a long straight string) is not zero – One trouble with thoughts about anything “infinitely long” is that, whatever the maths/theory might establish, you will never be able to provide physical “proof”.
Quote from: Bill S on 19/10/2018 14:03:31Quote from: Mad Aetherist I reckon that the gravitational field around an infinitely long straight wire (or a long straight string) is not zero – One trouble with thoughts about anything “infinitely long” is that, whatever the maths/theory might establish, you will never be able to provide physical “proof”.That a linear mass (wire/rod) has gravity dropping off as an inverse of radius (instead of inverse squared) derives directly from Newton's equations, and M-A gives a valid finite way to test this. It doesn't require infinite length.
A flat sheet has gravity that doesn't drop off at all. If Earth was flat and large enough, gravity would be 1 g all the way up.
Difference between an infinite plane, which, having no thickness, has no mass, and an infinite plate, which has mass and therefore a gravitational field since it is an infinite array of infinitesimal masses, each of which has a field, and gravitation is additive. Indeed it is exactly this additivity that makes it special.
Even though gravity is invisible apart from its effect on relative motion of bodies, gravitational energy is real. Gravitational waves prove beyond any reasonable doubt that GR is right on that specific topic. All energy produces a gravitational potential, gravity itself included. Many experiments proved the gravity-inertia equivalence, none proved the contrary. When you throw an object, you transfer some of your mass-energy to the object and the object increases its relativistic mass-energy by the same amount. Gravity included, relative to any inertial frame (or non accelerating observer).
affine connections