Physical Transformation AtlasPTA
Pathway · p-8200d7ab7e · candidate

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

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 route
    η_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

  1. 01
    nuclear → 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]
  2. 02
    Nuclear fission —produces→ Hot gasestablishedclaim record
    kinetic → 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]
  3. 03
    Hot gas —drives→ Thermal emissionestablishedclaim record
    thermal → radiative
    • a flame or a heated emitter radiating
    refs [5] [3]
  4. 04
    Thermal emission —converts into→ Lightestablishedclaim record
    radiative → 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. [1]
    O. Hahn, F. Strassmann. Über den Nachweis und das Verhalten der bei der Bestrahlung des Urans mittels Neutronen entstehenden Erdalkalimetalle (1939)
    Naturwissenschaften 27, 11–15 · doi:10.1007/BF01488241 · crossref ✓ 2026-09-19 · record
  2. [2]
    O. R. Frisch. Physical evidence for the division of heavy nuclei under neutron bombardment (1939)
    Nature 143, 276 · doi:10.1038/143276a0 · crossref ✓ 2026-09-19 · record
  3. [3]
    A. Bejan. Advanced Engineering Thermodynamics (4th ed.) (2016)
    Wiley · doi:10.1002/9781119245964 · crossref ✓ 2026-09-19 · record
  4. [4]
    U.S. Nuclear Regulatory Commission. Boiling Water Reactors — how a typical commercial BWR works (2025)
  5. [5]
    A. LaPotin, et al.. Thermophotovoltaic efficiency of 40% (2022)
    Nature 604, 287–291 · doi:10.1038/s41586-022-04473-y · crossref ✓ 2026-09-19 · record
  6. [6]
    P. T. Landsberg, G. Tonge. Thermodynamic energy conversion efficiencies (1980)
    Journal of Applied Physics 51, R1–R20 · doi:10.1063/1.328187 · crossref ✓ 2026-09-19 · record

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.