Geomagnetic Disturbance and HF Propagation
Geomagnetic Disturbance and HF Propagation
Correlating solar storms with what a UK Reverse Beacon actually hears
Geomagnetic storms are often reduced to shorthand phrases: “bands disturbed”, “conditions poor”, or simply “Kp too high”. While these descriptions are not wrong, they hide an important reality: geomagnetic disturbances affect HF propagation in structured, repeatable, and physically explainable ways.
Using CW Reverse Beacon data, covering late August 2024 through December 2025, spanning the peak and early decline of Solar Cycle 25, this article looks at how different HF bands respond during geomagnetically quiet periods versus disturbed periods, and how those responses align with well established solar terrestrial physics.
Geomagnetic storms are not “more solar cycle”
A useful starting point is to separate two solar influences that are sometimes confused.
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The solar cycle primarily affects HF through radiated output (EUV and soft X-rays), raising or lowering overall ionisation over weeks to years.
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Geomagnetic storms arise from solar wind–magnetosphere coupling, often driven by CMEs or high-speed solar wind streams and reorganise the ionosphere on timescales of minutes to hours.
During storms, the ionosphere does not simply lose ionisation. Instead, it becomes uneven, turbulent, and unstable, particularly at mid and high latitudes. HF propagation fails not because ionisation disappears, but because refraction becomes unreliable.
Storm signatures in Reverse Beacon data
Across multiple disturbed periods in the dataset, a consistent set of markers appear:
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Abrupt loss of 10m and 12m CW spots
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Increased variability on 15m and 17m
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Partial survival of 20m, often path-dependent
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Strong relative continuity on 40m, especially after sunset
These recurring patterns form a clear hierarchy that can be examined band by band.
Band-by-band response: quiet versus disturbed conditions
When many geomagnetically quiet days are compared with disturbed days, the relative behaviour of each HF band becomes clear. The table below summarises the typical response patterns observed in the RBN dataset, averaged qualitatively across multiple storm events.
| Band | Quiet geomagnetic conditions | Disturbed geomagnetic conditions |
|---|---|---|
| 10m | Regular openings near solar max | First to fail; openings short-lived |
| 12m | Frequent daytime activity | Rapid degradation; strong variability |
| 15m | Reliable daytime band | Patchy, direction-dependent |
| 17m | Stable mid-HF performance | Partially supported; fluctuating |
| 20m | Consistent day and evening | Often survives; increased fading |
| 30m | Steady, absorption-limited | Largely unchanged |
| 40m | Strong late-day and night-time | Often most reliable after sunset |
This qualitative hierarchy, high bands fail first, lower bands endure longest, appears repeatedly throughout the data and matches established ionospheric behaviour during geomagnetic disturbance.
Quantitative example: storm vs quiet spot-count ratios
To anchor this behaviour numerically, the table below compares actual CW spot counts received during a geomagnetically quiet period (7–8 October 2024) with those during a disturbed period (10–11 October 2024).
The ratio is defined simply as:
storm-period spots ÷ quiet-period spots
A value of 1.0 indicates no change.
Values below 1.0 indicate degradation, values above 1.0 indicate relative improvement.
| Band | Storm / Quiet ratio | What this shows |
|---|---|---|
| 10m | 0.71 | Clear degradation |
| 12m | 0.31 | Severe collapse |
| 15m | 0.41 | Strongly affected |
| 17m | 0.90 | Largely survives |
| 20m | 1.44 | Relative improvement |
| 30m | 0.74 | Moderately affected |
| 40m | 0.64 | Reduced, but still productive |
Several important points emerge:
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High bands collapse first and hardest, even during solar maximum.
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Mid-HF bands behave non-linearly - 17m survives where 15m does not.
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20m can improve in relative terms, as activity and usable propagation shift downward.
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40m does not improve, but it endures, continuing to support contacts when much of the spectrum is compromised.
These results are entirely consistent with storm-time ionospheric physics and are clearly reflected in the RBN data.
Case study highlights from the dataset
A few disturbed periods illustrate these effects particularly well:
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Mid-October 2024: abrupt collapse of 10m and 12m, unstable 15m, continued evening 40m activity
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Early November 2024: suppressed high bands, patchy 17m and 20m, strong post-sunset 40m
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Late March 2025: recovery-phase behaviour with persistent 40m and highly variable higher bands
Across all cases, the same hierarchy repeats: instability appears first at the top of the HF spectrum and works downward.
Why 40 metres anchors storm-time HF
Across every disturbed interval examined, 40m consistently shows:
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Persistence when higher bands fail
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Rapid improvement after sunset
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Reduced sensitivity to short-term ionospheric turbulence
This is not because conditions are better on 40m, but because the band is less demanding of ionospheric precision. During storms, robustness matters more than peak MUF and 40m provides exactly that.
Amateur observations and solar–terrestrial physics
The agreement between:
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recognised geomagnetically disturbed periods during Solar Cycle 25, and
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consistent band-by-band RBN behaviour
demonstrates that amateur CW networks respond coherently to the same physical drivers studied in professional space-weather research.
In effect, a long-running Reverse Beacon node functions as a fixed, mid-latitude ionospheric sensor.
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