Nuclear binding-energy difference → Useful heat
Nuclear binding-energy differenceNuclear fissionTemperature gradientHeat conductionHeat flowUseful heat
Epistemic state of the route
- known constituent relations
- 5 / 5 established or replicated · weakest constituent established
- 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 Heat exchanger · 3/5 relations shared
- route-level evidence
- 0 sources for the complete composition · 3 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 heat
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, filtered out by its applicabilityη ≤ 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 → thermalq = −κ · ∇T · thermal conductivity κ [W/(m K)]refs [3]
- 04
- 05thermal → thermal
- heat delivered at a temperature above the point of use
refs [3]
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 · 3
- [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)
Cite this route
Physical Transformation Atlas (2026). route p-4db87d8719: Nuclear binding-energy difference → Nuclear fission → Temperature gradient → Heat conduction → Heat flow → Useful heat. Dataset revision rbfbfcbb70e57 (hash of the canonical data). https://physical-transformation-atlas.wldud5192.workers.dev/path/4db87d8719
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.