A theory of electromagnetic and gravitational fields
โ Scribed by Clark Jeffries
- Publisher
- Elsevier Science
- Year
- 1991
- Tongue
- English
- Weight
- 475 KB
- Volume
- 4
- Category
- Article
- ISSN
- 0893-9659
No coin nor oath required. For personal study only.
โฆ Synopsis
Careful calculations using classical field theory show that if a macroscopic ball with uniform surface charge (say, a billiard ball with lE6 excess electrons) is released near the surface of the earth, it will almost instantaneously accelerate to relativistic speed and blow a hole in the ground. This absurd prediction is just the macroscopic version of the self-force problem for charged particles [l]. Furthermore, if one attempts to develop from electromagnetism a parallel theory for gravitation [2], the result is the same, self-acceleration. The basis of the new theory is a measure of energy density for any wave equation [3-51. Given any solution of any four-vector wave equation in spacetime (for example, the potentials (c-'&A) = (A",A',A2,A3) in 1 t e ec romagnetism), one can form the 16 first order partial derivatives of the vector components, with respect to the time and space variables (ct,z) = (IO, xl, x2 ,z3). The sum of the squares of the 16 terms is a natural energy function [6, p. 2831 (satisfying a conservation law g = -V . S). Such energy functions are routinely utilized by mathematicians as Lyapunov functions in the theory of stability of waves with boundary conditions. A Lagrangian using this sum leads to a new energy tensor for electromagnetic and gravitational fields, an alternative to that in [7].
๐ SIMILAR VOLUMES
The behaviour of a ``test'' electromagnetic field in the background of an exact gravitational plane wave is investigated in the framework of Einstein's general relativity. We have expressed the general solution to the de Rham equations as a Fourier-like integral. In the general case we have reduced