Chemical potential difference → Electrical work

Matrix context

D = disequilibrium row · C = coupling family column. A cell reads the state of the atlas for that pair.

D.05 × C.29 · Chemical potential difference × Thermochemicalfamily: ThermochemicalD.05 × C.08 · Chemical potential difference × Heat engine (thermomechanical)family: Heat engine (thermomechanical)D.05 × C.14 · Chemical potential difference × Electromagnetic inductionfamily: Electromagnetic induction

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 route
  η ≤ 1 − T_c/T_h for any heat engine between reservoirs at T_h and T_c
• Curzon–Ahlborn efficiency at maximum power · benchmark · listed, never decisive
  η_CA = 1 − √(T_c/T_h)

Steps

1. 01
   Chemical potential difference —drives→ Combustionestablishedclaim record

   chemical → thermal · loss to radiative

   • fuel, oxidiser and an ignition source; flame temperature 1500–2500 K

   gas · above ~700 K

   refs [1]
2. 02
   Combustion —produces→ Temperature gradientestablishedclaim record

   thermal → thermal

   refs [1]
3. 03
   Temperature gradient —drives→ Working-fluid expansion (heat-engine cycle)establishedclaim record

   thermal → mechanical · loss to thermal

   • a hot reservoir to heat the working fluid and a cold reservoir to condense or cool it

   temperature gradient required

   refs [1] [2]
4. 04
   Working-fluid expansion (heat-engine cycle) —produces→ Mechanical motionestablishedclaim record

   mechanical → mechanical · loss to thermal

   refs [1]
5. 05
   Mechanical motion —drives→ Electromagnetic inductionestablishedclaim record

   mechanical → electrical · loss to thermal

   • a magnet moving relative to a coil

   conductor required · magnetic field required

   refs [3] [4]
6. 06
   Electromagnetic induction —produces→ Charge carriersestablishedclaim record

   electrical → electrical · loss to thermal

   refs [3] [5]
7. 07
   Charge carriers —converts into→ Electrical workestablishedclaim record

   electrical → electrical · loss to thermal

   • carriers driven through an external load at the potential difference the source maintains

   refs [6]

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]
   A. Bejan. Advanced Engineering Thermodynamics (4th ed.) (2016)

   Wiley · doi:10.1002/9781119245964 · crossref ✓ 2026-09-19 · record
2. [2]
   G. Walker. Stirling Engines (1980)

   Oxford University Press · book, no DOI · record
3. [3]
   M. Faraday. Experimental researches in electricity (1832)

   Philosophical Transactions of the Royal Society 122, 125–162 · doi:10.1098/rstl.1832.0006 · crossref ✓ 2026-09-19 · record
4. [4]
   S. P. Beeby, et al.. A micro electromagnetic generator for vibration energy harvesting (2007)

   Journal of Micromechanics and Microengineering 17, 1257 · doi:10.1088/0960-1317/17/7/007 · crossref ✓ 2026-09-19 · record
5. [5]
   L. D. Landau, E. M. Lifshitz, L. P. Pitaevskii. Electrodynamics of Continuous Media (Course of Theoretical Physics, Vol. 8, 2nd ed.) (1984)

   Pergamon · book, no DOI · record
6. [6]
   N. W. Ashcroft, N. D. Mermin. Solid State Physics (1976)

   Holt, Rinehart and Winston · book, no DOI · record