Energy Aperture

Value chain · CLM-0069

In plain terms

The runaway threshold barely changes with atmospheric conditions. It is decided by the choice of frequency, not by the state of the atmosphere.

The claim as recorded

The thermal runaway threshold is insensitive to ionospheric conditions, varying by only about 11 per cent across a neutral temperature range of 170 to 210 K at 100 km altitude, because its dependence is only temperature to the power minus one half; it is set almost entirely by the design frequency.

T0 own calculation · medium confidence · as of 2026-09 · VER-901 CONFIRMED 2026-09-05 · VC06

Scope and limits

Applies only to the thermal runaway mechanism, not to self-focusing. And it is moot if CLM-0056 holds, since that records the runaway mechanism as having been refuted in 1981 as a transport coefficient artefact.

What it assumes

neutral temperature at 100 km spans roughly 170 to 210 K, which is provisional pending profile data

Where it comes from

This is the project's own working, shown in full:

CALC-007 Recovering the Duncan and Gordon relation, and evaluating its range
CALC-007 Recovering the Duncan and Gordon relation, and evaluating its range
At 2.45 GHz the relation gives 129 W/m2 at Tn = 170 K, 119 W/m2 at 200 K and 116 W/m2 at 210 K. CALC-007 shows the working. Applying the document's stated factor-of-two uncertainty to the 200 K case gives a band of 59 to 238 W/m2 at 2.45 GHz.
Related records
Answers question
QST-009 not published in this release
QST-010 not published in this release

Cite this

energyaperture.com/c/clm-0069

CLM-0069, Energy Aperture, as of 2026-09.