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one may also have a pressure term -∇p on the right-hand side of Eq. (7). In the vorticity-stream function formulation the pressure term in the modified Navier-Stokes (NS) equation [Eq. (7)] disappears because one considers a curl of the modified NS equati, has been discussed in Refs. 24, 25. We would also like to note that sound modes play only a minor role in spinodal decomposition as in the case of critical dynami, has been discussed by, and
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In general, one may also have a pressure term -∇p on the right-hand side of Eq. (7). In the vorticity-stream function formulation the pressure term in the modified Navier-Stokes (NS) equation [Eq. (7)] disappears because one considers a curl of the modified NS equation. This has been discussed in Refs. 24, 25. We would also like to note that sound modes play only a minor role in spinodal decomposition as in the case of critical dynamics. This has been discussed by J E. Farrell and O T. Valls, Phys. Rev. B42, 2353 (1990).
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37
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0000775026
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A somewhat different explanation for the transient surface roughening seen in experiments with a free-surface has been proposed by, and
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A somewhat different explanation for the transient surface roughening seen in experiments with a free-surface has been proposed by P. Keblinski, S K. Kumar, A. Maritan, J. Koplik and J R. Banavar, Phys. Rev. Lett.76, 1106 (1996).
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39
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85035240288
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The domain growth exponent in this regime is found to be n ≈0.4 in the presence of hydrodynamics 22
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The domain growth exponent in this regime is found to be n ≈0.4 in the presence of hydrodynamics 22.
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