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). Click to show full 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).
               
Click one of the above tabs to view related content.