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On the nature of the Rayleigh–Bénard convective instability

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Abstract

The initial stage of the Rayleigh–Bénard convective instability regarded as a nonequilibrium phase transition is reconstructed. Its mechanism is based on spinodal decomposition (diffusion separation).

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Author information

Authors and Affiliations

  1. Faculty of Mechanics and Mathematics, Moscow State University, Moscow, 119992, Russia

    E. V. Radkevich

  2. Turaerv Machine-Constructing Design Bureau “Soyuz”, Lytkarino, Moscow oblast, Russia

    E. A. Lukashev & N. N. Yakovlev

  3. Moscow State University of Civil Engineering, Moscow, 129337, Russia

    O. A. Vasil’eva

Authors
  1. E. V. Radkevich
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  2. E. A. Lukashev
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  3. N. N. Yakovlev
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  4. O. A. Vasil’eva
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Corresponding author

Correspondence to E. V. Radkevich.

Additional information

Original Russian Text © E.V. Radkevich, E.A. Lukashev, N.N. Yakovlev, O.A. Vasil’eva, 2017, published in Doklady Akademii Nauk, 2017, Vol. 475, No. 6, pp. 618–623.

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Radkevich, E.V., Lukashev, E.A., Yakovlev, N.N. et al. On the nature of the Rayleigh–Bénard convective instability. Dokl. Math. 96, 393–398 (2017). https://doi.org/10.1134/S1064562417040317

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  • DOI: https://doi.org/10.1134/S1064562417040317

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