Jonathan Scott
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There's a beautiful paper "On the Origin of Inertia" from 1953 by Dennis Sciama, which can be found online, which provides a specific explanation of inertia by drawing analogies between electromagnetism and gravity, combined with Mach's principle.
In electromagnetism, the electric field isn't just -\nabla \phi, but it also contains the term \partial A / \partial t where A is the vector potential. The vector potential due to an individual source is proportional to its velocity times the scalar potential, so the rate of change is proportional to the acceleration times the potential.
This means that if you accelerate nearby sources, this gives rise to an induced field. In corresponding gravitational terms, this means for example that a nearby accelerating mass gives rise to a tiny bit of "linear frame dragging", giving rise to an apparent field in the same direction, which tends to accelerate a test particle very slightly in the same direction.
Sciama points out that this could logically be extended to the whole universe, so if you consider the effect of accelerating the whole universe relative to a test mass, it will produce a significant force on the test mass in the same direction. If you then look at it from the other point of view, this says that if you accelerate a mass relative to the universe, you need to push against the force tending to resist that acceleration, which is what inertia is about. It also means that (in his simplified model) for the force to match F=ma the total potential \sum Gm/rc^2 for all sources in the universe must be equal to 1, so G becomes a function of the distribution of masses in the universe.
This is all very neat, and I feel there must be some truth in it, but unfortunately this model doesn't fit very will with the standard relativistic theory of gravity, Einstein's General Relativity. For a start, the electromagnetic analogy is very limited, as gravity is a tensor theory, and at the very least some factors of 2 or 4 are needed to make the equivalence work. I believe that in GR, according to Nordtvedt, it's the sum of 4Gm/rc^2 which would have to be equal to 1 to make linear frame dragging match inertia. However, as G is a fixed constant in GR, it is not clear how this could be made to work at all.
In electromagnetism, the electric field isn't just -\nabla \phi, but it also contains the term \partial A / \partial t where A is the vector potential. The vector potential due to an individual source is proportional to its velocity times the scalar potential, so the rate of change is proportional to the acceleration times the potential.
This means that if you accelerate nearby sources, this gives rise to an induced field. In corresponding gravitational terms, this means for example that a nearby accelerating mass gives rise to a tiny bit of "linear frame dragging", giving rise to an apparent field in the same direction, which tends to accelerate a test particle very slightly in the same direction.
Sciama points out that this could logically be extended to the whole universe, so if you consider the effect of accelerating the whole universe relative to a test mass, it will produce a significant force on the test mass in the same direction. If you then look at it from the other point of view, this says that if you accelerate a mass relative to the universe, you need to push against the force tending to resist that acceleration, which is what inertia is about. It also means that (in his simplified model) for the force to match F=ma the total potential \sum Gm/rc^2 for all sources in the universe must be equal to 1, so G becomes a function of the distribution of masses in the universe.
This is all very neat, and I feel there must be some truth in it, but unfortunately this model doesn't fit very will with the standard relativistic theory of gravity, Einstein's General Relativity. For a start, the electromagnetic analogy is very limited, as gravity is a tensor theory, and at the very least some factors of 2 or 4 are needed to make the equivalence work. I believe that in GR, according to Nordtvedt, it's the sum of 4Gm/rc^2 which would have to be equal to 1 to make linear frame dragging match inertia. However, as G is a fixed constant in GR, it is not clear how this could be made to work at all.
