Temperature gradient
Two regions at different temperatures. Heat flows down the gradient, and a fraction bounded by Carnot can be diverted into work.
Atlas record: 36 claims reference this disequilibrium — 26 established, 5 demonstrated, 3 replicated, 1 reported and 1 theoretically predicted.
Explorerelations · matrix context · routes · sources · cite
Relations
- sodium at 900–1300 K on the hot side of a β″-alumina electrolyte and a condenser at 400–700 K
- 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
- thermocapillary case: surface tension falls with temperature, so a temperature gradient along the interface drives flow toward the cold side
- a heavy metal with strong spin–orbit coupling (Pt, W) under a longitudinal temperature gradient; detected through the magnetoresistance of an adjacent magnetic insulator
- a membrane separating two reservoirs of the same liquid at different temperatures; the flow direction depends on the membrane–liquid interaction
- a ferrofluid whose magnetisation decreases with temperature, in a non-uniform magnetic field aligned with the temperature gradient
- a shape-memory alloy (NiTi) cycled between a hot reservoir above its austenite finish temperature and a cold one below its martensite finish temperature, under load
- a redox-active metal oxide (ceria, ferrites) reduced at 1400–1800 K, typically in a solar receiver, and re-oxidised by H₂O or CO₂ at 800–1200 K
- a spatial temperature gradient is applied across an insulating solid dielectric
- this claim represents the direct thermopolarization contribution; a signal established to arise through thermal expansion → strain gradient → flexoelectricity belongs to that longer pathway instead
- the solid spelling; the polar-liquid spelling is claim:temperature-drives-liquid-thermopolarization, with its own (simulation) evidence
- a polar molecular liquid is maintained under a spatial temperature gradient
- the response is the non-equilibrium polarization / electrostatic field of the liquid itself, not ionic thermodiffusion and not the pyroelectric response of an already ordered ferroelectric fluid (Máthé et al. 2022's ferroelectric-nematic thermomotor is that other coupling)
- simulation only: no experiment has measured the polarization of an ordinary polar liquid under a temperature gradient (pass 32 web search, not a route-search-v1 negative)
- a magnetised ferromagnet, metallic or insulating (YIG), under a temperature gradient
- an adjacent spin sink (heavy-metal layer) is needed for the usual electrical detection through inverse spin Hall conversion, not for the spin-Seebeck response itself
- a spatial temperature difference across a conductor or semiconductor
- a closed circuit of dissimilar materials, or a single material with ends at different temperatures
- a current flowing along a temperature gradient in a single conductor
- cathode hot enough that kT is a useful fraction of the work function (typically > 1500 K for metals, lower for low-work-function coatings)
- a cooler anode across a vacuum or caesium-vapour gap
- temperature gradient along the stack steeper than the critical gradient set by the acoustic pressure and displacement amplitudes
- a resonant gas column
- two identical electrodes in one redox electrolyte held at different temperatures
- a redox couple with large reaction entropy (ferri/ferrocyanide gives ≈ −1.4 mV/K)
- a battery chemistry whose open-circuit voltage changes with temperature by ≈ 1 mV/K
- charge at one temperature, discharge at the other, with heat recuperation between the two
- a liquid mixture or solution under a steady temperature gradient
- a magnetic field perpendicular to the temperature gradient; the transverse field is proportional to B and ∇T
- a magnetised ferromagnet or topological semimetal; no external field needed once magnetised
- a soft ferromagnet with its Curie temperature between the hot and cold reservoir temperatures (Gd ≈ 293 K)
- the element must be cycled between the reservoirs, so a heat-switch or motion is needed
- a hot reservoir to heat the working fluid and a cold reservoir to condense or cool it
- a ≈ 20 K difference between warm surface water and cold water from ~1000 m depth
- an emitter hotter than the surface it faces
- a bulk fluid flow connects the hotter and colder regions
- for forced circulation the flow may be supplied by an external pump rather than generated by buoyancy
- fragment and neutron kinetic energy thermalised in the fuel; the fuel runs hotter than the coolant
- energetic products (neutrons, alphas) deposit their kinetic energy in a blanket or the plasma, which then runs hotter than its surroundings
- the cooled surface sits a few kelvin below ambient air
- conversion of a heat flow between reservoirs at T_h and T_c into work or a non-thermal free energy; the bound is evaluated against a datum that records both temperatures
Matrix context
D = disequilibrium row · C = coupling family column. A cell reads the state of the atlas for that pair.
Enumerated routes through this · 542 (showing 24)
- Incandescent lamp2/2 est · demonstrated
- AMTEC cell1/3 est · demonstrated
- Thermocapillary micromotor3/3 est · demonstrated
- Shape-memory heat engine (mechanical)3/3 est · demonstrated
- Thermoelectric generator3/3 est · demonstrated
- Heat exchanger3/3 est · demonstrated
- Thermionic converter3/3 est · demonstrated
- Thermogalvanic cell3/3 est · demonstrated
- Thermally regenerative electrochemical cycle1/3 est · demonstrated
- Nernst–Ettingshausen generator3/3 est · demonstrated
- Anomalous Nernst thermopile3/3 est · demonstrated
- Steam Rankine cycle (shaft work)3/3 est · demonstrated
- Forced-circulation heat-delivery loop3/3 est · demonstrated
- Thermo-driven nanofluidic electrokinetic converter3/4 est · demonstrated
- Thermomagnetic hydrodynamic energy harvester3/4 est · demonstrated
- Thermal-osmosis electrokinetic generator5/5 est · demonstrated
- Thermomagnetic fluid engine5/5 est · demonstrated
- Shape-memory alloy heat engine5/5 est · demonstrated
- Spin Seebeck thermopile5/5 est · demonstrated
- Thermoacoustic piezoelectric harvester4/5 est · demonstrated
- Thermoacoustic triboelectric harvester4/5 est · demonstrated
- Thermoacoustic engine with linear alternator4/5 est · demonstrated
- Thermomagnetic generator4/5 est · demonstrated
- Steam Rankine plant5/5 est · demonstrated
Cited sources · 57
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- [4]L. E. Scriven, C. V. Sternling. The Marangoni Effects (1960)
- [5]Q. Dai et al.. Directional interfacial motion of liquids: Fundamentals, evaluations, and manipulation strategies (2021)
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- [8]V. M. Barragán, S. Kjelstrup. Thermo-osmosis in Membrane Systems: A Review (2017)
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- [10]R. E. Rosensweig. Ferrohydrodynamics (1985)
- [11]S. A. Suslov. Peculiarities of Convective Heat and Mass Transfer in Magnetic Nanofluids (2023)
- [12]K. Otsuka (ed.), C. M. Wayman (ed.). Shape Memory Materials (1998)
- [13]P. Kumar et al.. Shape memory alloy engine for high efficiency low-temperature gradient thermal to electrical conversion (2019)
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- [15]S. Abanades. Redox Cycles, Active Materials, and Reactors Applied to Water and Carbon Dioxide Splitting for Solar Thermochemical Fuel Production: A Review (2022)
- [16]M. Marvan. The electric polarization induced by temperature gradient and associated thermoelectric effects (1969)
- [17]A. K. Tagantsev. Pyroelectric, piezoelectric, flexoelectric, and thermal polarization effects in ionic crystals (1987)
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- [19]Y. Onishi et al.. Theory of Thermopolarization Effect (2025)
- [20]A. L. Kholkin, V. A. Trepakov, G. A. Smolenskii. Thermopolarization currents in dielectrics (1982)
- [21]F. Bresme et al.. Water Polarization under Thermal Gradients (2008)
- [22]J. Armstrong, F. Bresme. Temperature inversion of the thermal polarization of water (2015)
- [23]O. R. Gittus, P. Albella, F. Bresme. Polarization of acetonitrile under thermal fields via non-equilibrium molecular dynamics simulations (2020)
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- [31]W. Thomson. On a mechanical theory of thermo-electric currents (1851)
- [32]A. Bejan. Advanced Engineering Thermodynamics (4th ed.) (2016)
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- [37]M. F. Dupont, D. R. MacFarlane, J. M. Pringle. Thermo-electrochemical cells for waste heat harvesting – progress and perspectives (2017)
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Cite this entity
Physical Transformation Atlas (2026). entity disequilibrium:temperature-gradient: Temperature gradient. Dataset revision rbfbfcbb70e57 (hash of the canonical data). https://physical-transformation-atlas.wldud5192.workers.dev/e/disequilibrium/temperature-gradient
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