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Numerical methods
The different methods cannot be explained in greater detail here. The reader is referred to the applicable textbooks and publications.

The methods available when applied to the above mentioned objects have to comply with the criteria of giving valid results, in general the particular wavelength ratio to the size of the object. It turns out that all methods which are rigorous (e.g. MoM, FE,FD,FI), cannot solve the problem due to the extreme computer storage and computer time requirements. The most suitable methods are the ray method (GTD/UTD) for general cases and the current integration method (PO) for simpler cases. However, these are approximate methods and this application has to be controlled very carefully within the range of the approximation and its applicability, even though numbers and curves are generated. If not applied correctly, wrong results may be achieved.

The most capable numerical realizations (tools, computer programs) are relatively difficult to handle and require personnel with a high level of engineering know-how on

  • Antennas (antenna characteristics, radiators, arrays, polarisation, tolerances)
  • RF-technology (receivers, transmitters)
  • Wave propagation
  • Numerical techniques
  • System know-how and experience with the system to be analyzed.
If these numerical analysis tools in general and in particular in a simplified and approximate version, are distributed for public use some conditions should be met strictly. A detailed manual should be available for the user explaining in detail the
  • theory and approximations implied
  • applicability and limits for different objects and ground
  • expected range of accuracy.
In any case, the user should be trained adequately before applying the numerical methods being aware of the above mentioned conditions and assumptions. The user must be able to identify and interprete numerical artefacts uniquely for the applied method, e.g. the mentioned discontinuities for the GTD/UTD-method.

© NAVCOM Consult Mon Jul 13 01:39:07 CEST 2026