2010
DOI: 10.1134/s1063784210090069
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Instability of a thin layer of a magnetic fluid in a perpendicular magnetic field

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Cited by 11 publications
(14 citation statements)
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“…The characteristic spacing in the hexagonal pattern (instability wavenumber) follows an exponential decay with the thickness of the ferrofluid layer and a logarithmic increase with the applied field. 62 Consequently, the large wavenumbers of the instability-generated patterns in Fig. 6 result from the limited critical film thickness in a typical drop-casting experiment, i.e.…”
Section: Ferrohydrodynamic Instabilitiesmentioning
confidence: 97%
“…The characteristic spacing in the hexagonal pattern (instability wavenumber) follows an exponential decay with the thickness of the ferrofluid layer and a logarithmic increase with the applied field. 62 Consequently, the large wavenumbers of the instability-generated patterns in Fig. 6 result from the limited critical film thickness in a typical drop-casting experiment, i.e.…”
Section: Ferrohydrodynamic Instabilitiesmentioning
confidence: 97%
“…The last assumption is confirmed by the results of Cebers (1997), who for a close problem showed that smearing of the diffusion front shifts the most dangerous mode to a longer wavelength. The result obtained rather resembles the behaviour of the free interface of a magnetic fluid, on which the Rosensweig instability (Cowley & Rosensweig 1967) develops upon instantaneous switching on of a magnetic field of various magnitudes (Bashtovoi, Krakov & Reks 1985; Dikansky, Zakinyan & Mkrtchyan 2010; Zakinyan, Mkrtchyan & Dikansky 2016). With an increase in the value of the switched-on magnetic field, the length of the most rapidly developing wavelength in this case significantly decreased.…”
Section: Numerical Results and Discussionmentioning
confidence: 64%
“…Increasing the magnetic field strength further leads to a breakup of liquid ridges into conical peaks arranged into a hexagonal pattern. This hexagonal pattern of peaks is analogous to the pattern arising in a normal magnetic field [9][10][11][12], but in this case the conical peaks are inclined to layer plane and the hexagons are stretched along the horizontal field component. The value of the external magnetic field strength at which the transition to a hexagonal pattern of peaks takes place was measured (the second critical field, H c2 ).…”
Section: Methodsmentioning
confidence: 67%
“…Peculiarities of thin layers instability is also a subject of several recent theoretical researches [6][7][8]. As to experiments in this area, it seems that only works [9][10][11][12] can be mentioned. The dependencies of the critical 1 magnetic field strength and critical wave number on the thickness of the magnetic fluid layer have been measured.…”
Section: Introductionmentioning
confidence: 99%
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