The Nature of Cold Fusion (Cold Fusion Made Simple)
Edmund Storms
Abstract and summary · read the original at the source
In one page
Edmund Storms, at Kiva Labs in Santa Fe, has spent decades measuring cold fusion, and here he tries to say plainly how it works rather than why — a distinction he draws with a pilot who flies well without knowing the theory of lift. His picture has three layers. The ordinary crystal lattice cannot host fusion, because its own rules hold the nuclei too far apart; it is the hydrogen reservoir and nothing more. The reaction needs a second and rare condition he calls the nuclear active environment: gaps or cracks of a particular width, wider than the spacing between hydrogen atoms in the lattice but too narrow for hydrogen molecules to form. Inside those gaps, hydrogen nuclei and electrons occasionally assemble into a shared structure that can fuse. The practical payoff is a recipe — embed inert particles of a chosen size in palladium, and the metal swells around them as it absorbs hydrogen, opening gaps of a width you can calculate in advance. He then lists the measurements that would confirm the model or kill it.
Why it matters hereChapter 12 needs a mechanism that says where in a metal the reaction happens and how to put it there deliberately, and this is the clearest statement of one: the active site is a gap of critical width, and gaps can be engineered. Chapter 1’s ladder gets the falsifiable half — Storms turns his model into specific isotope and neutron predictions anyone with a cell can check.
What it claims
01Cold fusion needs three chemical relationships in sequence, not one: the ordinary crystal structure, which cannot host the reaction because its own rules hold the nuclei too far apart and which serves only as the hydrogen source; a rare nuclear active environment that forms physically outside the crystal structure; and, at a few random places inside it, a nuclear active structure of hydrogen nuclei and electrons sharing a wave function — an assembly Storms compares to the charge clusters Ken Shoulders reported and to ball lightning.Section 2, General Summary of the Model; Section 2.3
Published and peer-reviewed02The active site is a gap of critical width — wider than the distance between hydrogen atoms in the crystal but narrower than the size at which the hydrogen molecule would form, because molecule formation competes with the less stable active structure — and once such a gap has been populated with hydrogen it becomes chemically stable, so the reaction thereafter runs independently of the deuterium-to-palladium ratio.Sections 2.2.1 and 2.2.2
Published and peer-reviewed03Gaps can be manufactured rather than waited for: add inert particles of a chosen size to palladium, and hydrogen absorption swells the metal around the unchanged particle, opening a gap equal to the fractional expansion times the particle dimension divided by two — the expansion running as 0.055 times the hydrogen-to-palladium ratio up to 0.6, and as 0.011 plus 0.038 times that ratio from 0.6 to 1.0 — so that a 0.35 micrometre particle should switch on near a ratio of 0.2 and a 0.1 micrometre particle near 0.8; calcium oxide, silicon dioxide and boron nitride particles have already produced consistent behaviour.Section 2.2.3, Figures 3 and 4
Designed, not yet built04Storms proposes that every hydrogen isotope pair fuses by the same route — an electron joins the assembly, making a heavier isotope of hydrogen that then beta-decays — giving deuterium plus deuterium into helium-4 at 23.8 megaelectronvolts, hydrogen plus deuterium into tritium and then helium-3 at 4.9, and hydrogen plus hydrogen into deuterium at 1.9, and he draws the checkable consequences: pure deuterium should make no tritium, pure protium should make tritium slowly, and neutrons should rise as the tritium-to-deuterium ratio approaches unity.Section 2.4, Table 1; Section 2.5, numbered implications 1 to 6
What to watch05The reported tritium-to-neutron ratio in these experiments sits many orders of magnitude above the value near unity that hot fusion gives, and the energetic ion spectra measured by Karabut and, eight years later, by Storms and Scanlan with different detectors in different laboratories agree: separate ion energies evenly spaced by 0.417 megaelectronvolts, mostly between about 1 and 6 megaelectronvolts, with intensity falling exponentially as energy rises.Section 2.4, Figure 7; Section 2.5, Figures 8 to 11
Published and peer-reviewed06Excess power rises with temperature as a straight line in the logarithm of power against inverse temperature, with the same slope across four samples of different deuterium content, giving an activation energy of 0.303 electronvolts per atom close to the 0.230 electronvolts per atom for diffusion of deuterium in palladium deuteride — so what temperature controls is resupply of hydrogen to the active site, and a sample carried from an electrolytic cell into deuterium gas produced similar power at the same temperatures.Section 2.6, Figures 12 and 13
Published and peer-reviewed
The way in
https://doi.org/10.70923/001c.124949The article itself is paginated as Journal of Condensed Matter Nuclear Science 38 (2023) 130 to 146 and carries the line ‘© 2023 ICCF. All rights reserved’, while the DOI record dates it 2024. The journal’s own article metadata records no open licence, so this page carries the summary, the claims and the author’s own abstract, and sends the reader to the full text at the source.
How to cite it
Edmund Storms (2024) The Nature of Cold Fusion (Cold Fusion Made Simple). doi:10.70923/001c.124949
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