Abstract
It is shown that a stationary space containing a black hole is a solution of the Brans-Dicke field equations if and only if it is a solution of the Einstein field equations. This implies that when the star collapses to form a black hole, it loses that fraction (about 7%) of its measured gravitational mass that arises from the scalar interaction. This mass loss is in addition to that caused by emission of scalar or tensor gravitational radiation. Another consequence is that there will not be any scalar gravitational radiation emitted when two black holes collide.
Similar content being viewed by others
References
Hawking, S.W.: Commun. math. Phys.25, 152–166 (1972).
Nordtvedt, K. Jr.: Phys. Rev.169, 1017 (1968).
Weber, J.: Phys. Rev. Letters22, 1320 (1969).
—— Nuovo Cimento4 B, 197 (1971).
Gibbons, G.W., Hawking, S.W.: Phys. Rev. (1971) (to be published).
Charman, W.N.,et al.: Nature228, 346 (1970).
Bahcall, J.N.: Phys. Rev. Letters26, 662 (1971).
Dicke, R.H.: Phys. Rev.125, 2163 (1962).
Carter, B.: J. Math. Phys.10, 70 (1969).
Penrose, R.: Phys. Rev. Letters10, 66 (1963).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Hawking, S.W. Black holes in the Brans-Dicke. Commun.Math. Phys. 25, 167–171 (1972). https://doi.org/10.1007/BF01877518
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01877518