Abstract
The problem of the field equations and the equations of motion in general
relativity theory is now sufficiently clarified. The equations of motion can
be deduced from pure field equations by treating matter as singularities,
[2; 3], or from field equations with the energy momentum tensor [4].
Recently two papers appeared in which the problem of the coordinate system
was considered [5; 8]. The two papers are in general agreement as far as the
role of the coordinate system is concerned. Yet there are some differences
which require clarification.
Publisher
Canadian Mathematical Society
Cited by
16 articles.
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