Nuclear binding-energy difference → Light
Nuclear binding-energy differenceNuclear fissionHot gasThermal emissionLight
Epistemic state of the route
- known constituent relations
- 4 / 4 established or replicated · weakest constituent established
- constituent maturity floor
- K4 · experimentally observed
- search for this exact route
- Exact composition search: reviewed 2026-09-21 — partial; None found in the runs made (a partial, never a protocol-complete negative): the composite-name form reaches the nuclear light bulb programme — spectral and start-up analyses, RF and DC-arc radiant-environment simulations, transparent-wall tests and designs for in-reactor tests of small models — and none of it is a fissioning gas radiating light as its product; the fission-plus-plasma experiments the second reader knows (the Langley plasma focus; the Walters & Schneider neutron-field discharge) do not establish the fission → radiation handoff either. Whether any in-reactor light-bulb model test was run before the programme ended is the open question. Inconclusive as a route search until the Scholar and Semantic Scholar runs exist.
- recorded-pathway overlap
- shares relations, in order, with Boiling-water reactor direct-steam plant · 2/4 relations shared
- route-level evidence
- 0 sources for the complete composition · 6 cited by the constituent steps
- boundaries and interfaces
- BOUNDARY unknown · no scoped condition requirements recorded
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.07 · Nuclear binding-energy difference × Thermophotovoltaicfamily: Thermophotovoltaic
Literature search for this exact composition
None found in the runs made (a partial, never a protocol-complete negative): the composite-name form reaches the nuclear light bulb programme — spectral and start-up analyses, RF and DC-arc radiant-environment simulations, transparent-wall tests and designs for in-reactor tests of small models — and none of it is a fissioning gas radiating light as its product; the fission-plus-plasma experiments the second reader knows (the Langley plasma focus; the Walters & Schneider neutron-field discharge) do not establish the fission → radiation handoff either. Whether any in-reactor light-bulb model test was run before the programme ended is the open question. Inconclusive as a route search until the Scholar and Semantic Scholar runs exist.
- Analytical study of the spectral radiant flux emitted from the fuel region of a nuclear light bulb engine (1970) · theory only · United Aircraft 1970: the spectral radiant flux of the fuel region computed, by title — analysis.
- Theoretical investigation of the radiant emission spectrum from the fuel region of a nuclear light bulb engine (1969) · theory only · United Aircraft 1969: the fuel region's emission spectrum computed, by title — theory.
- Initial radio-frequency gas heating experiments to simulate the thermal environment in a nuclear light bulb reactor (1969) · wrong driver · United Aircraft 1969: RF-heated gas standing in for the fissioning fuel — the radiant thermal environment reproduced without fission (the second reader: not a source-variant, since the conversion's driver is absent).
- Results of experiments to simulate radiant heating of propellant in a nuclear light bulb engine using a D-C arc radiant energy source (1970) · wrong driver · United Aircraft 1970: a DC-arc radiant source heating propellant in place of the fissioning fuel, by title — the radiant handoff demonstrated with a non-fission source.
- Development of a high intensity RF radiant energy source for simulating the thermal environment of the nuclear light bulb reactor (1971) · wrong driver · United Aircraft 1971: an RF radiant source built to simulate the reactor's thermal environment, by title.
- Analytical design and performance studies of nuclear furnace tests of small nuclear light bulb models (1972) · insufficient information · United Aircraft 1972: designs for in-reactor (Nuclear Furnace) tests of small light-bulb models — whether any in-reactor test was carried out before the programme ended is the one question that decides this route, unread.
- High temperature UF6 RF plasma experiments applicable to uranium plasma core reactors (1979) · wrong driver · NASA-era 1979: UF₆ plasma heated by RF, applicable to plasma-core reactors, by title — the plasma made without fission.
- Nuclear characteristics of a fissioning uranium plasma test reactor with light-water cooling (1973) · proposal only · 1973: the nuclear characteristics of a proposed fissioning-uranium-plasma test reactor, by title — a design.
- Nuclear light bulb (1991) · review only · 1991: a nuclear light bulb overview, by title.
6055 indexed works reported across the queries, 265 unique retrieved; nobody has read them for a qualifying demonstration. A person can screen this frozen list and promote it to a reviewed record without re-running the query.
- OAcomposite-name222 reported · 100 retrieved
- OAdriver-mechanism:12909 reported · 100 retrieved
- OAdriver-mechanism:12909 reported · 50 retrieved
- OAmechanism-pair:1-215 reported · 15 retrieved
- OAwhole-chain0 reported · 0 retrieved
- OAdemonstration-precision0 reported · 0 retrieved
Planned runs NOT run in this bundle (engine unavailable): search:2026-09-21-p-8200d7ab7e/s2-cn (semantic-scholar); search:2026-09-21-p-8200d7ab7e/s2-dm1 (semantic-scholar); search:2026-09-21-p-8200d7ab7e/s2-mp12 (semantic-scholar); search:2026-09-21-p-8200d7ab7e/s2-wc (semantic-scholar); search:2026-09-21-p-8200d7ab7e/s2-dp (semantic-scholar).
Protocol route-search-v1: a frozen index run changes only the search state; only a reviewed record can say that a demonstration was or was not found.
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).
- Visible-band fraction of thermal emission · formula-bound · hard, applies to this routeη_vis ≤ ∫₃₈₀ⁿᵐ⁷⁸⁰ⁿᵐ B_λ(λ, T) dλ / σT⁴ — the share of a thermal emitter's radiated power that Planck's distribution places in the visible band at the emitter temperature
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
- fission heating produces a vapour or gas working fluid in a DIRECTLY heated, same-circuit configuration: the reactor coolant itself boils in the vessel and its steam goes to the turbine (a boiling-water reactor), or the fissioning or fission-heated gas is the working medium (a gas-core or fissioning-plasma reactor)
- not a pressurised-water reactor: there fission heats a pressurised liquid whose heat crosses a steam generator into a separate secondary circuit — the heat exchanger, not the core, makes the turbine's steam, and that topology belongs to the system layer, never hidden inside this claim (pass 38)
refs [3] [4] - 03thermal → radiative
- a flame or a heated emitter radiating
refs [5] [3] - 04radiative → radiative · loss to radiative
- incandescence at > 2000 K
refs [6] [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 · 6
- [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]U.S. Nuclear Regulatory Commission. Boiling Water Reactors — how a typical commercial BWR works (2025)
- [5]A. LaPotin, et al.. Thermophotovoltaic efficiency of 40% (2022)
- [6]P. T. Landsberg, G. Tonge. Thermodynamic energy conversion efficiencies (1980)
Cite this route
Physical Transformation Atlas (2026). route p-8200d7ab7e: Nuclear binding-energy difference → Nuclear fission → Hot gas → Thermal emission → Light. Dataset revision rbfbfcbb70e57 (hash of the canonical data). https://physical-transformation-atlas.wldud5192.workers.dev/path/8200d7ab7e
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.