The Gravitational Field of a Disk

Physics

Scientific paper

Rate now

  [ 0.00 ] – not rated yet Voters 0   Comments 0

Details

87

Scientific paper

The general solution of the static field equations of general relativity is given for a disk of "counterrotating" dust particles. The only nonvanishing components of the energy-momentum tensor are T00 and Tχχ, which are assumed to have δ-function singularities on the disk. Two representative families of solutions are considered, and it is shown that, for these solutions, physical considerations severely limit the strength of the gravitational potentials. The first family has surface density proportional to some power of 1-ρ2. Th requirement that the velocity of the dust particles should not exceed c places a bound on the gravitational red-shift of z=1.5803 for these models. The second family is that of the uniformly rotating disks defined by v2=ρ2ω2e-4φ. Bardeen has pointed out that these disks can have arbitrarily large red-shifts without violating the velocity condition. However, it is shown that their red-shift cannot exceed 1.9015 before their binding energy becomes negative. This work suggests that the largest gravitational red-shift to which counter-rotating dust disks can give rise is of order of magnitude 1.

No associations

LandOfFree

Say what you really think

Search LandOfFree.com for scientists and scientific papers. Rate them and share your experience with other people.

Rating

The Gravitational Field of a Disk does not yet have a rating. At this time, there are no reviews or comments for this scientific paper.

If you have personal experience with The Gravitational Field of a Disk, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and The Gravitational Field of a Disk will most certainly appreciate the feedback.

Rate now

     

Profile ID: LFWR-SCP-O-1829809

  Search
All data on this website is collected from public sources. Our data reflects the most accurate information available at the time of publication.