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- Line-of-sight (Figure 467): The most straightforward interference propagation situation is when a line of sight (LoS) transmission path exists under normal (i.e. well‑mixed) atmospheric conditions. However, an additional complexity can come into play when subpath diffraction causes a slight increase in signal level above that normally expected. Also, on all but the shortest paths (i.e. paths longer than about 5 km) signal levels can often be significantly enhanced for short periods of time by multipath and focusing effects resulting from atmospheric stratification (see Figure 463468).
- Diffraction (Figure 467): Beyond LoS and under normal conditions, diffraction effects generally dominate wherever significant signal levels are to be found. For services where anomalous short-term problems are not important, the accuracy to which diffraction can be modelled generally determines the density of systems that can be achieved. The diffraction prediction capability must have sufficient utility to cover smooth‑earth, discrete obstacle and irregular (unstructured) terrain situations.
- Tropospheric scatter (Figure 467): This mechanism defines the “background” interference level for longer paths (e.g. more than 100-150 km) where the diffraction field becomes very weak. However, except for a few special cases involving sensitive receivers or very high power interferers (e.g. radar systems), interference via troposcatter will be at too low a level to be significant.
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Figure 467: Long-term interference propagation mechanisms (Source: ITU-R P.452)Anchor F467 F467
- Surface ducting (Figure 463468): This is the most important short-term propagation mechanism that can cause interference over water and in flat coastal land areas, and can give rise to high signal levels over long distances (more than 500 km over the sea). Such signals can exceed the equivalent “free‑space” level under certain conditions.
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