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  • 2103.12765v2

    Rights statement: © 2021 American Physical Society

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Continuous non-equilibrium transition driven by the heat flow

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Continuous non-equilibrium transition driven by the heat flow. / Zhang, Yirui; Litniewski, Marek; Makuch, Karol et al.
In: Physical Review E, Vol. 104, No. 2, 024102, 02.08.2021.

Research output: Contribution to Journal/Magazine › Journal article › peer-review

Harvard

Zhang, Y, Litniewski, M, Makuch, K, Zuk, PJ, Maciolek, A & Holyst, R 2021, 'Continuous non-equilibrium transition driven by the heat flow', Physical Review E, vol. 104, no. 2, 024102. https://doi.org/10.1103/PhysRevE.104.024102

APA

Zhang, Y., Litniewski, M., Makuch, K., Zuk, P. J., Maciolek, A., & Holyst, R. (2021). Continuous non-equilibrium transition driven by the heat flow. Physical Review E, 104(2), Article 024102. https://doi.org/10.1103/PhysRevE.104.024102

Vancouver

Zhang Y, Litniewski M, Makuch K, Zuk PJ, Maciolek A, Holyst R. Continuous non-equilibrium transition driven by the heat flow. Physical Review E. 2021 Aug 2;104(2):024102. doi: 10.1103/PhysRevE.104.024102

Author

Zhang, Yirui ; Litniewski, Marek ; Makuch, Karol et al. / Continuous non-equilibrium transition driven by the heat flow. In: Physical Review E. 2021 ; Vol. 104, No. 2.

Bibtex

@article{0128f4032b1644878d261651faa4a3aa,
title = "Continuous non-equilibrium transition driven by the heat flow",
abstract = " We discovered an out-of-equilibrium transition in the ideal gas between two walls, divided by an inner, adiabatic, movable wall. The system is driven out-of-equilibrium by supplying energy directly into the volume of the gas. At critical heat flux, we have found a continuous transition to the state with a low-density, hot gas on one side of the movable wall and a dense, cold gas on the other side. Molecular dynamic simulations of the soft-sphere fluid confirm the existence of the transition in the interacting system. We introduce a stationary state Helmholtz-like function whose minimum determines the stable positions of the internal wall. This transition can be used as a paradigm of transitions in stationary states and the Helmholtz-like function as a paradigm of the thermodynamic description of these states. ",
keywords = "cond-mat.stat-mech",
author = "Yirui Zhang and Marek Litniewski and Karol Makuch and Zuk, {Pawel J.} and Anna Maciolek and Robert Holyst",
note = "{\textcopyright} 2021 American Physical Society ",
year = "2021",
month = aug,
day = "2",
doi = "10.1103/PhysRevE.104.024102",
language = "English",
volume = "104",
journal = "Physical Review E",
issn = "2470-0045",
publisher = "American Physical Society",
number = "2",

}

RIS

TY - JOUR

T1 - Continuous non-equilibrium transition driven by the heat flow

AU - Zhang, Yirui

AU - Litniewski, Marek

AU - Makuch, Karol

AU - Zuk, Pawel J.

AU - Maciolek, Anna

AU - Holyst, Robert

N1 - © 2021 American Physical Society

PY - 2021/8/2

Y1 - 2021/8/2

N2 - We discovered an out-of-equilibrium transition in the ideal gas between two walls, divided by an inner, adiabatic, movable wall. The system is driven out-of-equilibrium by supplying energy directly into the volume of the gas. At critical heat flux, we have found a continuous transition to the state with a low-density, hot gas on one side of the movable wall and a dense, cold gas on the other side. Molecular dynamic simulations of the soft-sphere fluid confirm the existence of the transition in the interacting system. We introduce a stationary state Helmholtz-like function whose minimum determines the stable positions of the internal wall. This transition can be used as a paradigm of transitions in stationary states and the Helmholtz-like function as a paradigm of the thermodynamic description of these states.

AB - We discovered an out-of-equilibrium transition in the ideal gas between two walls, divided by an inner, adiabatic, movable wall. The system is driven out-of-equilibrium by supplying energy directly into the volume of the gas. At critical heat flux, we have found a continuous transition to the state with a low-density, hot gas on one side of the movable wall and a dense, cold gas on the other side. Molecular dynamic simulations of the soft-sphere fluid confirm the existence of the transition in the interacting system. We introduce a stationary state Helmholtz-like function whose minimum determines the stable positions of the internal wall. This transition can be used as a paradigm of transitions in stationary states and the Helmholtz-like function as a paradigm of the thermodynamic description of these states.

KW - cond-mat.stat-mech

U2 - 10.1103/PhysRevE.104.024102

DO - 10.1103/PhysRevE.104.024102

M3 - Journal article

VL - 104

JO - Physical Review E

JF - Physical Review E

SN - 2470-0045

IS - 2

M1 - 024102

ER -