Energy Aperture

Value chain · CLM-0500

In plain terms

The same formula for how much microwave power a beam can carry before it destabilises the upper atmosphere gives 425 watts per square metre at one textbook set of conditions and a typical 189 across thousands of real radar measurements. That is not two methods disagreeing; it is one method fed different starting numbers.

The claim as recorded

One governing relation, the Perkins-and-Goldman-derived threshold with its Ne^-3 and Te^+4 scaling, gives a 5.8 GHz self-focusing threshold of 425 W/m2 when Usui 2008 evaluates it at a single nominal condition (Ne 1e12 m^-3, Te 1500 K), and a median of 189 W/m2 when it is evaluated over the 1,827 of 22,705 measured Millstone Hill mid-latitude radar pairs that satisfy the domain condition at 5.8 GHz. The factor of 2.25 between them is explained by the inputs alone: a factor of 1.98 comes from the in-domain median density of 1.255e12 m^-3 being above Usui's nominal 1e12, and the same implementation reproduces Usui's figure to within 0.1 per cent at Usui's own inputs.

T2 peer-reviewed analysis, model or thesis · medium confidence · as of 2008; 2026-09 (comparison) · VER-1341 CONFIRMED 2026-09-19 · VC06, VC07

Scope and limits

The two routes use different input plasma conditions (Usui's stated reference point vs measured mid-latitude radar distributions), so the disagreement partly reflects real condition-dependence, not only method disagreement; the self-focusing threshold spans several orders of magnitude across day/night and solar-cycle conditions (claims.md ~1716), so neither figure should be read as a single fixed limit. THESE TWO FIGURES MAY NOT BE CITED AS MUTUAL CORROBORATION OR AS AN INDEPENDENT CHECK ON ONE ANOTHER, condition added 2026-09-04. They are one relation evaluated at two input sets, and a point value cannot be compared with a distribution median as though the two were competing estimates of the same quantity. A genuine independent check would require a threshold relation not derived from Perkins and Goldman, and synthesis/calcs.md records that none was found. The 1,827-pair count is not printed in CALC-014, which gives 8.0 per cent of 22,705 rows in domain at 5.8 GHz (1,816 to 1,827 depending on rounding), so the exact count is consistent with CALC-014 but not recomputed from it (VER-1341 CONFIRMED 2026-09-19).

What it assumes

Both routes assume the same underlying Perkins-and-Goldman-derived governing relation and the same Ne^-3, Te^+4-type scaling; the Ne^-3 exponent itself is confirmed by no source (synthesis/decision.md).

Where it comes from

SRC-124 Interactions between Microwave Beam and Ionosphere, 2008
(Usui 2008), reproduced to better than 0.1 per cent by an implementation made here (claims.md ~2483: "32.01 and 424.73 watts per square metre"); claims.md ~2301: "Median threshold 919 W/m2 at 2.45 GHz and 189 W/m2 at 5.8 GHz."

Basis: W/m2, self-focusing threshold at 5.8 GHz; one relation at two input sets, one a point evaluation and one a distribution median

Related records
Answers question
QST-001 not published in this release

Cite this

energyaperture.com/c/clm-0500

CLM-0500, Energy Aperture, as of 2008; 2026-09 (comparison).

Connected records

Other published records linked to this one. A list, not a judgement.

Also from SRC-124
CLM-0104A separate Japanese review worked out the same threshold from the original paper and got 32 and 425 watts per square metre. My own...
CLM-0105A third party looked at the 230 watt per square metre design figure and said self-focusing may happen at 2.45 gigahertz but not at 5.8...
CLM-0168In this 2008 Japanese review, the absorption figures of under 1% normally and up to about 10% at increased solar activity are not tied to...
CLM-0169The 2008 Japanese review that gives the well-known 32 and 425 watts-per-square-metre self-focusing thresholds only ever says self-focusing...