freesurface:jcp
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freesurface:jcp [2010/11/24 17:39] Kirill Nikitin |
freesurface:jcp [2014/04/22 08:21] (current) |
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| [[http://www.inm.ras.ru/research/_media/movies:zalesak:256_32_16_particles.avi|{{:movies:zalesak:256_32_16_particles.png?270x180|Zalesak's disk}}]] | [[http://www.inm.ras.ru/research/_media/movies:zalesak:256_32_16_particles.avi|{{:movies:zalesak:256_32_16_particles.png?270x180|Zalesak's disk}}]] | ||
| - | * The breaking dam problem (also known as collapsing water column): The schematic apparatus from J. Martin, W. Moyce, Philos.Trans.R.Soc.Lond.Ser.A, V. 244 (1952) and animated numerical solutions 1) without particles method 2) with particles | + | * The breaking dam problem (also known as collapsing water column): The schematic apparatus from J. Martin, W. Moyce, Philos.Trans.R.Soc.Lond.Ser.A, V. 244 (1952) and animated numerical solutions 1) velocity field 2) without particles method 3) with particles |
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| + | {{:movies:bd:bd_scheme_1.jpg?270x180|Breaking dam scheme}} | ||
| + | [[http://www.inm.ras.ru/research/_media/movies:bd:bd.avi|{{:movies:bd:bd.png?270x180|Breaking dam}}]] | ||
| + | [[http://www.inm.ras.ru/research/_media/movies:bd:bd1.avi|{{:movies:bd:bd.jpg?270x180|Breaking dam}}]] | ||
| + | [[http://www.inm.ras.ru/research/_media/movies:bd:bd2.avi|{{:movies:bd:bd.jpg?270x180|Breaking dam}}]] | ||
| See [1] for comparative analysis of numerical and experimental data. | See [1] for comparative analysis of numerical and experimental data. | ||
| * The oscillating droplet problem (see linear analysis in H. Lamb, Hydrodynamics, Cambridge University Press, 1932): At initial moment the fluid is in rest, but the mean curvature of the surface is not constant, and an unbalanced surface tension force causes droplet oscillation. The fluid motion is solely driven by the surface tension forces. | * The oscillating droplet problem (see linear analysis in H. Lamb, Hydrodynamics, Cambridge University Press, 1932): At initial moment the fluid is in rest, but the mean curvature of the surface is not constant, and an unbalanced surface tension force causes droplet oscillation. The fluid motion is solely driven by the surface tension forces. | ||
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| + | [[http://www.inm.ras.ru/research/_media/movies:drop:osc_drop.avi|{{:movies:drop:osc_drop.png?270x180|Oscillating droplet}}]] | ||
| See [1] for the discussion of the physical relevance of the numerical solutions. | See [1] for the discussion of the physical relevance of the numerical solutions. | ||
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| + | [[|More free surface flows animations]] | ||
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| + | Contributers: | ||
| + | * [[http://dodo.inm.ras.ru/nikitink/portfolio.html|Kirill Nikitin]] (PhD student at [[http://www.inm.ras.ru/inm_en_ver/index.htm|INM RAS]]) | ||
| + | * [[http://www.mathcs.emory.edu/~molshan|Maxim Olshanskii]] (professor at [[http://www.msu.ru/|MSU]]) | ||
| + | * Artem Suleimanov (student at [[http://www.msu.ru/|MSU]]) | ||
| + | * Kirill Terekhov (PhD student at [[http://www.inm.ras.ru/inm_en_ver/index.htm|INM RAS]]) | ||
| + | * Yuri Vassilevski (professor at [[http://www.inm.ras.ru/inm_en_ver/index.htm|INM RAS]]) | ||
freesurface/jcp.1290620391.txt.gz · Last modified: 2014/04/22 08:19 (external edit)
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