Static Axisymmetric Interior Solution in General Relativity

1967 ◽  
Vol 163 (5) ◽  
pp. 1373-1376 ◽  
Author(s):  
J. J. J. Marek

Formulae are given for the field of a sphere of constant gravitational mass density.


1961 ◽  
Vol 2 (2) ◽  
pp. 206-208 ◽  
Author(s):  
N. W. Taylor

The theory of relativity shows that the times measured by two observers will in general be different if they are in relative motion, so that their respective times between any two coincidences will differ. Bergmann [1] has investigated the problem of a particle moving in a small simple harmonic motion in a static gravitational field, and has found that the time difference for this particle and an observer at rest becomes zero whenever the particle passes through the centre and limits of its swing. This problem will now be dealt with in a different manner, using Schwarzschild's interior solution of the gravitational equations. The exterior solution for a point mass is not suitable in the present case, due to the singularity of the field at a point in the path of the particle.


We find an exact cylindrically symmetric stationary exterior solution of the Einstein-Maxwell equations. We then match this solution smoothly onto an interior solution for rotating charged dust found earlier by the author. The solution thus obtained is regular and well behaved inside the matter. Such matched solutions are rare either for the Einstein or Einstein-Maxwell equations. Some properties of the solution are discussed.


1988 ◽  
Vol 130 (1) ◽  
pp. 1-6 ◽  
Author(s):  
Chongming Xu ◽  
Chun Li Shen ◽  
Xuejun Wu

2017 ◽  
Vol 9 (6) ◽  
pp. 8 ◽  
Author(s):  
Valery V. Vasiliev ◽  
Leonid V. Fedorov

The paper is concerned with the spherically symmetric static problem of the General Relativity Theory (GRT). The classical interior solution of this problem found in 1916 by K. Schwarzschild for a fluid sphere is generalized for a linear elastic isotropic solid sphere. The GRT equations are supplemented with the equation for the stresses which is similar to the compatibility equation of the theory of elasticity and is derived using the principle of minimum complementary energy for an elastic solid. Numerical analysis of the obtained solution is undertaken.


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