Nuclear binding-energy difference → Electrical work
Nuclear binding-energy differenceRadioactive decayBeta particlesRadioisotope heatingTemperature gradientIonic thermoelectric effectIonic currentElectrical work
Epistemic state of the route
- known constituent relations
- 7 / 7 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 relations, in order, with Radioluminescent (beta-photovoltaic) nuclear battery · 2/7 relations shared
- route-level evidence
- 0 sources for the complete composition · 4 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.33 · Nuclear binding-energy difference × Thermodiffusivefamily: Thermodiffusive
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 → nuclearradioisotope requiredrefs [1]
- 02nuclear → nuclear
- beta emitters such as tritium, Ni-63, Pm-147, Sr-90
refs [1] - 03nuclear → thermal
- beta particles stopped within the source and its cladding; in practice RTG heat comes from alpha emitters (see the alpha claim)
radioisotope requiredrefs [1] - 04thermal → thermalrefs [1]
- 05thermal → electrical · loss to thermal
- an electrolyte (liquid, gel or polymer) under a temperature difference; ionic Seebeck coefficients of 1–10 mV/K arise from differential thermodiffusion of cations and anions, without electrode redox entropy
temperature gradient requiredrefs [2] [3] - 06electrical → electricalrefs [3]
- 07electrical → electrical · loss to thermal
- electrodes exchange the ionic current for an electronic current through the external load
refs [4]
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 · 4
- [1]M. A. Prelas, et al.. A review of nuclear batteries (2014)
- [2]M. Bonetti et al.. Huge Seebeck coefficients in nonaqueous electrolytes (2011)
- [3]D. Zhao, A. Würger, X. Crispin. Ionic thermoelectric materials and devices (2021)
- [4]A. J. Bard, L. R. Faulkner. Electrochemical Methods: Fundamentals and Applications (2nd ed.) (2001)
Cite this route
Physical Transformation Atlas (2026). route p-20b93670fc: Nuclear binding-energy difference → Radioactive decay → Beta particles → Radioisotope heating → Temperature gradient → Ionic thermoelectric effect → Ionic current → Electrical work. Dataset revision rbfbfcbb70e57 (hash of the canonical data). https://physical-transformation-atlas.wldud5192.workers.dev/path/20b93670fc
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.