Nuclear binding-energy difference → Electrical work
Nuclear binding-energy differenceNuclear fissionTemperature gradientAlkali-metal thermal-to-electric conversionIonic currentElectrical work
Epistemic state of the route
- known constituent relations
- 3 / 5 established or replicated · weakest constituent demonstrated
- constituent maturity floor
- K4 · experimentally observed
- search for this exact route
- Not assessed — complete composition not searched.
- recorded-pathway overlap
- shares its closing relations with AMTEC cell · 3/5 relations shared
- route-level evidence
- 0 sources for the complete composition · 5 cited by the constituent steps
- boundaries and interfaces
- BOUNDARY compatible · no region transition
Explorematrix context · physics checks · steps · route evidence · constituent evidence · cite
Matrix context
D = disequilibrium row · C = coupling family column. A cell reads the state of the atlas for that pair.
D.20 × C.27 · Nuclear binding-energy difference × Nuclear heatfamily: Nuclear heatD.20 × C.21 · Nuclear binding-energy difference × Electrochemicalfamily: Electrochemical
Typed bounds on this route
Every limit the atlas holds for this route, as constraint records: reached through bounded_by claims on the route's own entities. Hard bounds (an upper bound or a formula) decide the thermodynamic-bound check above; benchmarks, constitutive relations and resource limits are listed and never decisive. No prose limit exists anywhere (pass 42).
- Carnot limit · formula-bound · hard, applies to this routeη ≤ 1 − T_c/T_h for any heat engine between reservoirs at T_h and T_c
Steps
- 01nuclear → kinetic · loss to radiative
- for neutron-induced fission: a fissionable nuclide and an incident neutron in an energy range with non-zero fission cross-section
- critical geometry is required only for a self-sustaining chain reaction; a moderator is reactor-design dependent
About 200 MeV per event, almost all as fragment kinetic energy (Frisch 1939); thermalisation is a separate step.refs [1] [2] - 02kinetic → thermal · loss to radiative
- fragment and neutron kinetic energy thermalised in the fuel; the fuel runs hotter than the coolant
refs [2] [3] - 03thermal → electrical · loss to thermal
- sodium at 900–1300 K on the hot side of a β″-alumina electrolyte and a condenser at 400–700 K
above ~700 K · liquidrefs [4] - 04electrical → electricalrefs [4]
- 05electrical → electrical · loss to thermal
- electrodes exchange the ionic current for an electronic current through the external load
refs [5]
Evidence for the complete composition · 0
No source on record for this exact composition. The sources below support the individual steps, not the route as a whole.
Evidence for the constituent relations · 5
- [1]O. Hahn, F. Strassmann. Über den Nachweis und das Verhalten der bei der Bestrahlung des Urans mittels Neutronen entstehenden Erdalkalimetalle (1939)
- [2]O. R. Frisch. Physical evidence for the division of heavy nuclei under neutron bombardment (1939)
- [3]A. Bejan. Advanced Engineering Thermodynamics (4th ed.) (2016)
- [4]T. Cole. Thermoelectric energy conversion with solid electrolytes (1983)
- [5]A. J. Bard, L. R. Faulkner. Electrochemical Methods: Fundamentals and Applications (2nd ed.) (2001)
Cite this route
Physical Transformation Atlas (2026). route p-56e3e83558: Nuclear binding-energy difference → Nuclear fission → Temperature gradient → Alkali-metal thermal-to-electric conversion → Ionic current → Electrical work. Dataset revision rbfbfcbb70e57 (hash of the canonical data). https://physical-transformation-atlas.wldud5192.workers.dev/path/56e3e83558
Ids and matrix addresses are stable across revisions; the revision hash identifies the exact canonical files the record was compiled from and is meta.data_hash in every /api export. Reuse terms: see the license field in any export.