Free-electron density Skywaves |
The ionosphere enables skywave ![]() Figure 1: Skywave, LOS and ground wave |
The ionosphere is a layer of the upper atmosphere detailed in Figure 2. Let's focus on the mesosphere and ionosphere, which are located between 50 to 700 kilometers above Earth's surface:
EUV sunlight ionizes atoms and molecules, releasing free electrons and ions that combine to form plasma. Hence the name Ionosphere.
The ionosphere is divided into regions at altitudes from 48 to 600 kilometers above the earth's surface.
This figure shows ionospheric regions, labeled D, E, F1, and F2, with an additional label F on the night side. It highlights the variation in ionosphere regions between day and night, with the day side on the left and the night side on the right. This visual representation helps understand how the ionosphere's structure changes with the time of day.
These regions are distinguished by their free-electron densities.
The above graph is based on a review from U.C.Berkeley by Bob Brown Ph.D, NM7M (SK) ↗
HF radio waves aimed at the inosphere can be bounced, allowing for global communication channels.

Figure 6 shows different modes of radio wave propagation in the ionosphere, including ionospheric tilt, chordal mode, ducted mode, sporadic E, F skip, 1F1E, and 1F1Es1F. It highlights how radio waves interact with the E and F regions, illustrating their travel paths over long distances.
Summary:
This page explains how the ionosphere enables HF radio communication by forming plasma layers (Figures 1–2) and organizing into distinct regions—D, E, and F (Figure 4). Changes in electron density with altitude and time (Figure 5) allow various skywave propagation modes, including skip, ducted, and chordal paths (Figure 6).
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