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a) Positive mass attracts negative mass.
Newton's shell theorem addresses the field strength inside the boundary.
It is well known that the speed of light goes to zero at the event horizon of a Schwarzschild black hole. You can prove this to yourself by solving the metric for a radially in-falling photon, for which proper time is identical to zero. The result is:c=co(1-rs/r)The Shapiro effect exemplifies this phenomenon.What happens to an in-falling mass is less obvious because the speed of proper time is a function of velocity:dT/dt=sqrt((1-rs/r)(1-(v/c)2))
The mass density of a back hole defines the local space-time profile. This profile is not defined by the observer, any more than the gravity of the sun and the pressures it exerts is dependent on the observer. Mass is an invariant.
If you fell into a black hole, the pressures would kill you long before we could run any test.
You could define a negative energy, but only for kinetic energy and if the energy were expressed as a vector rather than a scalar. Negative rest energy would be a very bizarre concept indeed.
Eventually all this can end up in group theory. Especially considering the Lorentz and Poincare groups. Group theory isn't my favourite pastime.https://en.m.wikipedia.org/wiki/Fundamental_group