Skip to content
DraconiticResearch
Search Sources API
203,203 studies31 sourcesUpdated 50 min ago
PreprintCC BY 4.0arXiv

A microscopic heat engine with many hidden variables

Abstract

Microscopic motors are commonly monitored through a single mechanical coordinate, whereas the chemical, conformational, or rotational cycles that sustain their motion remain unresolved. Mechanical stall is defined by the vanishing of the mean observed velocity; this scalar condition, however, does not generally imply thermodynamic reversibility. We analyze an overdamped Brownian motor in which one observed coordinate is coupled to several internal phases through a single shared interaction potential. Because the transmitted force and the reaction torques derive from the same energy, the resulting rank-one reciprocal structure yields an exact pointwise identity between the observed and hidden probability currents. This identity provides an exact expression for the entropy production at stall for an arbitrary periodic interaction. In particular, a positive current-square dissipation in the mechanical channel, defined from the full stationary state through the coupling-coordinate-resolved local velocity, determines together with the stall load the collective hidden current projected onto the coupling direction. The stationary one-coordinate marginal current nevertheless vanishes identically at stall; consequently, the stationary marginal density and mean displacement current do not determine this dissipation. Hidden currents orthogonal to the coupling direction dissipate without affecting the observed motion and generate an irreducible contribution that cannot be inferred from the rank-one mechanical channel.

Related

  1. Emergent Sparsity: How Many Effective Variables Survive Coarse-Graining in AlphaEarth Embeddings?
    Johannes Hirn
    arXivPreprintCC BY-NC-ND 4.0Full textGeophysics & seismologyStatistical & nonlinear physicsarXiv
  2. Turning a superconducting diode into a Feynman ratchet to realize a nanoscale heat engine
    Konstantinos Kontogeorgiou, İnanç Adagideli, Géraldine Haack +1
    arXivPreprintarXiv licenceFull textCondensed matterQuantum physics & quantum informationarXiv
  3. Ideal heat engine cycles at maximal efficiency -- the ideal gas and beyond
    Gregory Behrendt, Sebastian Deffner
    arXivPreprintCC BY 4.0Full textStatistical & nonlinear physicsarXiv
  4. Thermodynamic bound on the Fano factor of a coherent thermoelectric heat engine
    Nahual Sobrino, Rosario Fazio, Matteo Acciai
    arXivPreprintarXiv licenceFull textCondensed matterarXiv
  5. Finite-Bandwidth Protection of a Three-Level Quantum Heat Engine Against Parasitic Heat Leaks
    Gilberto Aparecido Prataviera, Marcos César de Oliveira
    arXivPreprintCC BY 4.0Full textQuantum physics & quantum informationarXiv
BibTeX
@misc{taye2026microscopic,
  title = {{A microscopic heat engine with many hidden variables}},
  author = {Mesfin Asfaw Taye},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.18941},
  eprint = {2609.18941},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.18941},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - A microscopic heat engine with many hidden variables
AU  - Mesfin Asfaw Taye
PY  - 2026
DA  - 2026/09/01
PB  - arXiv
DO  - 10.48550/arxiv.2609.18941
UR  - https://arxiv.org/abs/2609.18941
AB  - Microscopic motors are commonly monitored through a single mechanical coordinate, whereas the chemical, conformational, or rotational cycles that sustain their motion remain unresolved. Mechanical stall is defined by the vanishing of the mean observed velocity; this scalar condition, however, does not generally imply thermodynamic reversibility. We analyze an overdamped Brownian motor in which one observed coordinate is coupled to several internal phases through a single shared interaction potential. Because the transmitted force and the reaction torques derive from the same energy, the resulting rank-one reciprocal structure yields an exact pointwise identity between the observed and hidden probability currents. This identity provides an exact expression for the entropy production at stall for an arbitrary periodic interaction. In particular, a positive current-square dissipation in the mechanical channel, defined from the full stationary state through the coupling-coordinate-resolved local velocity, determines together with the stall load the collective hidden current projected onto the coupling direction. The stationary one-coordinate marginal current nevertheless vanishes identically at stall; consequently, the stationary marginal density and mean displacement current do not determine this dissipation. Hidden currents orthogonal to the coupling direction dissipate without affecting the observed motion and generate an irreducible contribution that cannot be inferred from the rank-one mechanical channel.
ER  -