I. Introduction
The functioning of numerous radio-engineering systems is based on the use of ground radio waves that propagate along the earth’s surface and are not influenced by the ionosphere. The ground wave has the advantage, first, in the stability of its amplitude-phase structure and in the possibility of propagation over long distances in the LF-MF radio wave bands. Many works are devoted to the problems of propagation of ground radio waves, among which the first works of A. Sommerfeld [1], G. Weil, J. Watson, V.A. Fock [2]. In the middle and late 20th century, the theory of radio wave propagation continued to be developed by other researchers. They obtained practical models for calculating electromagnetic fields. G.I. Makarov [3] and J. Wait [4] made the most important contribution to solving the problem for the model of the medium, which has inhomogeneities in the depth of the earth’s structure. Propagation over highly inductive paths, which are possible only with inhomogeneous media, at some distances from the source may be characterized by the fact that the field level will exceed the field level above a perfectly conducting surface. This effect was experimentally confirmed by the researchers of the Laboratory of Electromagnetic Diagnostics of the Institute of Physical Materials Science (Ulan-Ude, Russia) when measuring the field levels in the HF frequency range on the ice of a salt lake [5],[6]. In addition, at some distances, the field can change non-monotonically due to the presence of SEW. Previously, such effects were associated only with waves reflected from the ionosphere.