A non-static Einstein-Maxwell solution
J Carminati; C B G McIntosh; J Carminati; Math. Dept., Monash Univ., Clayton, Vic., Australia; C B G McIntosh; Math. Dept., Monash Univ., Clayton, Vic., Australia
Журнал:
Journal of Physics A: Mathematical and General
Дата:
1980-03-01
Аннотация:
The Einstein-Maxwell field equations are solved completely when the line element has the form ds<sup>2</sup>=exp(2h)dt<sup>2</sup>-exp(2A)(dx<sup>2</sup>+dy<sup>2</sup>)-exp(2B)dz<sup>2</sup> where h, A and B are functions of t only, and is thus non-static. The metric admits a four-parameter group of motions. The Weyl tensor is type D and the electromagnetic field is non-null.
351.4Кб