Einstein’s Gravitation for Machian Relativism of Nonlocal Energy-Charges

• Published in: International journal of theoretical physics Vol. 47; no. 5; pp. 1261 - 1269
• Main Author: Bulyzhenkov-Widicker, I. E.
• Format: Journal Article
• Language: English
• Published: Boston Springer US 01.05.2008; Springer Nature B.V
• Subjects: Einstein equations; Electromagnetic radiation; Elementary Particles; Energy; Gravitation; Mathematical and Computational Physics; Physics; Physics and Astronomy; Quantum Field Theory; Quantum Physics; Relativism; Relativity; Tensors; Theoretical; Gravitational four-potentials; Unification; Continuous particle; Non-empty space; Non-dual carriers; 3D flatness; Nonlocal energy-charge
• ISSN: 0020-7748; 1572-9575
• DOI: 10.1007/s10773-007-9559-z

Tetrads require six metric bounds and energy-to-energy gravitation in the 1913 tensor generalization of the SR four-vector and the scalar four-interval. Only four energy-momentum components of the 1915 source equation can be relevant to flatspace gravitation of overlapping nonlocal carriers of energy-charges. New singularity-free metric equally works for the Einstein-Grossmann geodesic motion and for the r −4 elementary source in non-empty flatspace with the local time dilatation. The GR energy integral of the nonlocal radial (astro)carrier is finite and determines its active/passive gravitational charges. The SR reference for self-contained Einstein’s relativity replaces the constant masses with their GR energies in the 1686 universal law of gravitation for the undivided world ensemble of overlapping radial matter. Gravitational/inertial energy-charges of nonlocal carriers depend on their global time-varying interactions with other elementary energy-charges that quantitatively address Machian relativism for gravitation and inertia. Electromagnetic waves change the gravitational/inertial energy-charge that can be tested in the Solar system. The non-empty space paradigm admits geometrization of the radial particle in the 1915 Einstein equation and suggests the similar field-energy nature for the distributed electric charge.