Abstract

We consider lattice Universes with spatial topologies T×T×TT\times T\times T,   T×T×R  \; T\times T\times R\; and   T×R×R\; T\times R\times R. In the Newtonian limit of General Relativity, we solve the Poisson equation for the gravitational potential in the enumerated models. In the case of point-like massive sources in the T×T×TT\times T\times T model, we demonstrate that the gravitational potential has no definite values on the straight lines joining identical masses in neighboring cells, i.e. at points where masses are absent. Clearly, this is a nonphysical result since the dynamics of cosmic bodies is not determined in such a case. The only way to avoid this problem and get a regular solution at any point of the cell is the smearing of these masses over some region. Therefore, the smearing of gravitating bodies in NN-body simulations is not only a technical method but also a physically substantiated procedure. In the cases of   T×T×R  \; T\times T\times R\; and   T×R×R\; T\times R\times R topologies, there is no way to get any physically reasonable and nontrivial solution. The only solutions we can get here are the ones which reduce these topologies to the T×T×TT\times T\times T one.

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