Nuclear binding-energy difference → Useful heat
Nuclear binding-energy differenceNuclear fusionTemperature gradientThermal emissionPhotonsPhotothermal absorptionHeat flowUseful heat
Epistemic state of the route
- known constituent relations
- 5 / 7 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 relations, in order, with Thermophotovoltaic conversion · 2/7 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.07 · Nuclear binding-energy difference × Thermophotovoltaicfamily: ThermophotovoltaicD.20 × C.20 · Nuclear binding-energy difference × Photothermalfamily: Photothermal
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
- Visible-band fraction of thermal emission · formula-bound · hard, filtered out by its applicabilityη_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
- Landsberg limit · formula-bound · hard, filtered out by its applicabilityη ≤ 1 − (4/3)(T_c/T_s) + (1/3)(T_c/T_s)⁴ for conversion of blackbody radiation at T_s with a sink at T_c; 93.3 % at 6000 K / 300 K
Steps
- 01nuclear → kinetic · loss to radiative
- for a power-producing D–T thermonuclear plasma: ion temperatures of order 10 keV and a sufficient density–confinement product (Lawson); these are power-balance conditions, not prerequisites for an individual fusion reaction
plasma · above ~700 KFusion reactions and target-level fusion energy release are experimentally demonstrated (target gain > 1 at NIF, 2022–2024); net electrical output from a fusion power plant is not.refs [1] [2] [3] - 02kinetic → thermal · loss to radiative
- energetic products (neutrons, alphas) deposit their kinetic energy in a blanket or the plasma, which then runs hotter than its surroundings
refs [2] [3] - 03thermal → radiative
- an emitter hotter than the surface it faces
refs [4] [5] - 04
- 05
- 06
- 07thermal → thermal
- heat delivered at a temperature above the point of use
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 · 5
- [1]H. A. Bethe. Energy production in stars (1939)
- [2]J. D. Lawson. Some criteria for a power producing thermonuclear reactor (1957)
- [3]H. Abu-Shawareb, et al. (Indirect Drive ICF Collaboration). Achievement of target gain larger than unity in an inertial fusion experiment (2024)
- [4]A. Bejan. Advanced Engineering Thermodynamics (4th ed.) (2016)
- [5]P. T. Landsberg, G. Tonge. Thermodynamic energy conversion efficiencies (1980)
Cite this route
Physical Transformation Atlas (2026). route p-0df797a7e5: Nuclear binding-energy difference → Nuclear fusion → Temperature gradient → Thermal emission → Photons → Photothermal absorption → Heat flow → Useful heat. Dataset revision rbfbfcbb70e57 (hash of the canonical data). https://physical-transformation-atlas.wldud5192.workers.dev/path/0df797a7e5
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.