Electromagnetic contribution to gravitational mass of a current-conducting channel

Details Electromagnetic contribution to gravitational mass of a current-conducting channel Electromagnetic contribution to gravitational mass of a current-conducting channel

Jan 2000

adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2000phrvd..61b4004m&link_type=abstract

Physical Review D (Particles, Fields, Gravitation, and Cosmology), Volume 61, Issue 2, 15 January 2000, id.024004

Physics

4

Einstein-Maxwell Spacetimes, Spacetimes With Fluids, Radiation Or Classical Fields

Scientific paper

The analysis of electromagnetic contribution to the total mass of a strong current channel is conducted on the basis of Einstein's equations of general theory of relativity. The current dependence of the ratio R of the contribution of the magnetic field to the contribution of the charges has a maximum. While the current is small (from the point of view of its influence on the metric) the ratio R grows with the current. Then R reaches its maximum, and in the region of a strong current up to the collapse boundary it is a decreasing function of the current. If the drift velocity is not too small, the magnetic contribution can be many orders of magnitude higher than the sum of masses of the charges.

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