Physical Transformation AtlasPTA
Pathway · p-ace7db2cbb · extends a recorded pathway

Temperature gradient → Electrical work

Temperature gradientThermal expansionMechanical stress or strainVillari effectChanging magnetic fluxElectromagnetic inductionCharge carriersElectrical 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 Bimetallic-strip piezoelectric harvester · 2/7 relations shared
route-level evidence
0 sources for the complete composition · 8 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.01 × C.08 · Temperature gradient × Heat engine (thermomechanical)family: Heat engine (thermomechanical)D.01 × C.15 · Temperature gradient × Magnetostrictivefamily: MagnetostrictiveD.01 × C.14 · Temperature gradient × 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
  • Onsager–Casimir reciprocity · constitutive-relation · listed, never decisive
    L_ij(B) = ε_i ε_j L_ji(−B): the cross-coefficients of coupled linear transport are equal up to the time-reversal parities ε of the variables and reversal of the magnetic field; L_ij = L_ji is the zero-field, even-parity case

Steps

  1. 01
    thermal → mechanical
    refs [1] [2]
  2. 02
    mechanical → mechanical
    • non-uniform thermal expansion is mechanically incompatible across adjacent regions of a solid, or is constrained by an adjoining material or structure, producing a strain or stress gradient; the constraining region may be the cooler part of the same continuous specimen rather than a separate stiffer body
    solid
    refs [3] [2]
  3. 03
    mechanical → magnetic · loss to thermal
    • a magnetostrictive material under a bias field and cyclic stress
    solid · ferromagnet required
    refs [4] [5]
  4. 04
    magnetic → magnetic
    refs [5] [6]
  5. 05
    magnetic → electrical · loss to thermal
    ℰ = −dΦ/dt · rate of change [1/s]
    • the changing flux threads a conducting loop
    conductor required
    refs [7] [6]
  6. 06
    electrical → electrical · loss to thermal
    refs [7] [6]
  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 [8]

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 · 8

  1. [1]
    A. Bejan. Advanced Engineering Thermodynamics (4th ed.) (2016)
    Wiley · doi:10.1002/9781119245964 · crossref ✓ 2026-09-19 · record
  2. [2]
    S. Iwakiri, Y. Miyata, T. Mori. Observation of universal thermopolarization effect in insulators (2026)
    arXiv:2605.17224 (17 May 2026), National Institute for Materials Science, Tsukuba · arxiv.org/abs/2605.17224 · record
  3. [3]
    J. F. Nye. Physical Properties of Crystals: Their Representation by Tensors and Matrices (1985)
    Oxford University Press · book, no DOI · record
  4. [4]
    E. Villari. Ueber die Aenderungen des magnetischen Moments, welche der Zug und das Hindurchleiten eines galvanischen Stroms in einem Stabe von Stahl oder Eisen hervorbringen (1865)
    Annalen der Physik 202, 87–122 · doi:10.1002/andp.18652020906 · crossref ✓ 2026-09-19 · record
  5. [5]
    L. Wang, F. G. Yuan. Vibration energy harvesting by magnetostrictive material (2008)
    Smart Materials and Structures 17, 045009 · doi:10.1088/0964-1726/17/4/045009 · crossref ✓ 2026-09-19 · record
  6. [6]
    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
  7. [7]
    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
  8. [8]
    N. W. Ashcroft, N. D. Mermin. Solid State Physics (1976)
    Holt, Rinehart and Winston · book, no DOI · record

Cite this route

Physical Transformation Atlas (2026). route p-ace7db2cbb: Temperature gradient → Thermal expansion → Mechanical stress or strain → Villari effect → Changing magnetic flux → Electromagnetic induction → Charge carriers → Electrical work. Dataset revision rbfbfcbb70e57 (hash of the canonical data). https://physical-transformation-atlas.wldud5192.workers.dev/path/ace7db2cbb

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.