Abstract
The equations of Rainich's “already unified field theory” are investigated for the typeG 3 II acting on the spatially homogeneous hypersurfacesx 0=constant. Two solutions of a non-static electromagnetic field for the above case are presented here by using the exterior differential calculus. The space-time admits a three-parameter continuous group of motions, the minimum invariant varieties being the geodesically parallel parametric surfacesx 1=constant,x 2=constant andx 3=constant orthogonal tox 0=constant at points of the geodesics.
Similar content being viewed by others
References
Rainich G. Y.: Trans. Am. Math. Soc.27 (1925) 106.
Misner C. W., Wheeler J. A.: Ann. Phys. (N. Y.)2 (1957) 525.
Witten L.: Colloque sur la Théorie de la Relativité, Centre Belge de Recherches Mathématiques, Brussels, 1959, p. 59–77.
Witten L.: Phys. Rev.115 (1959) 1, 206.
Witten L.: Phys. Rev.120 (1960) 635.
Raychaudhuri A. K.: Ann. Phys. (N. Y.)11 (1960) 501.
Rosen G.: J. Math. Phys.3 (1962) 313.
Rosen G.: Phys. Rev. B136 (1964) 297.
Brill D. R.: Phys. Rev. B133 (1964) 845.
Datta B. K.: Ann. Phys. (N. Y.)12 (1961) 295.
Datta B. K.: Ann. Phys. (N. Y.)15 (1961) 403.
Datta B. K.: Relativity and Gravitation, Gordon and Breach, London 1970, p. 111–121.
Datta B. K.: Nuovo Cim.36 (1965) 109.
Bera K., Datta B. K.: J. Phys. A1 (1968) 650.
Bera K., Datta B. K.: GRG5 (1974) 483.
De N., Datta B. K.: Phys. Rev. D3 (1971) 1280.
Rawal J. J., Datta B. K.: Proc. Internat. Symposium on Relativity and Unified Field Theory, S. N. Bose Inst. of Phys. Scs., Calcutta, 1975–76, p. 291–292.
Taub A. H.: Ann. Math.53 (1951) 472.
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Bhattacharyya, K.K., Datta, D. & Datta, B.K. Non-static electromagnetic field in general relativity VI. Czech J Phys 32, 980–986 (1982). https://doi.org/10.1007/BF01597171
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01597171