I have shown in two recently published reports, how one can arrive at field equations of gravitation, that are in agreement with the postulate of general relativity,

*i.e.*which in their general form are covariant in respect to arbitrary substitutions of space-time variables.

The line of development was as follows. At first I found equations, that contain Newton's theory as approximation and that are covariant in respect to arbitrary substitutions of the determinant 1. Afterwards I found, that those equations in general correspond to covariant ones, if the scalar of the energy tensor of "matter" vanishes. The coordinate system had to be specialized in accordance with the simple rule, that is made to 1, whereby the equations of the theory experience an eminent simplification. In the course of this, however, one had to introduce the hypothesis, that the scalar of the energy tensor of matter vanishes.

Recently I find now, that one is able to dispense with hypothesis concerning the energy tensor of matter, if one fills in the energy tensor of matter into the field equations in a somehow different way than it was done in my two earlier reports. The field equations for vacuum, upon which I based the explanation of the perihelion motion of mercury, remain untouched by this modification. I give the complete consideration again at this place, so that the reader is not forced to uninterruptedly consultate the earlier reports.

From the well known Riemannian covariant of fourth rank, the following covariant of second rank is derived:

(1) |

(1a) |

(1b) |

(2) |

(3) |

(3a) |

(4) |

If "matter" exists in the considered space, then its energy tensor appears on the right hand side of (2) or (3). We put

(2a) |

(5) |

(6) |

(3a) |

(7) |

(7a) |

(8) |

(8a) |

If we multiply (6) by and sum over the indices and , then we obtain after simple calculation

(9) |

(8b) |

*l.c.*.

Furthermore one derives instead of equation (22)

*l.c.*, in the way as it is given there by the aid of the energy equation, the relations:

(10) |

By that, the general theory of relativity as a logical building is eventually finished. The relativity postulate in its general form that makes the space-time coordinates to physically meaningless parameters, is directed with stringent necessity to a very specific theory of gravitation that explains the perihelion motion of mercury. However, the general relativity postulate offers nothing new about the essence of the other natural processes, which wasn't already taught by the special theory of relativity. My opinion regarding this issue, recently expressed at this place, was erroneous. Any physical theory equivalent to the special theory of relativity, can be included in the general theory of relativity by means of the absolute differential calculus, without that the latter gives any criterion for the admissibility of that theory.