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1997
DOI: 10.1051/jp1:1997186
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Macro-Organized Patterns in Ferrofluid Layer: Experimental Studies

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Cited by 61 publications
(54 citation statements)
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“…Similar patterns were observed previously [18][19][20][21][22]. When a magnetic fluid is confined with an immiscible nonmagnetic liquid between closely spaced horizontal glass plates (Hele-Schaw cell) and subjected to an external magnetic field perpendicular to the plate, labyrinths and hexagonal arrays of columns are formed [19,[23][24][25][26][27][28][29]. These patterns are produced at the interface between the magnetic and nonmagnetic phases, and they are explained in terms of competition between the magnetic and surface energy.…”
Section: Mesoscopic Structures Obtained By Applying a Magnetic Field supporting
confidence: 73%
“…Similar patterns were observed previously [18][19][20][21][22]. When a magnetic fluid is confined with an immiscible nonmagnetic liquid between closely spaced horizontal glass plates (Hele-Schaw cell) and subjected to an external magnetic field perpendicular to the plate, labyrinths and hexagonal arrays of columns are formed [19,[23][24][25][26][27][28][29]. These patterns are produced at the interface between the magnetic and nonmagnetic phases, and they are explained in terms of competition between the magnetic and surface energy.…”
Section: Mesoscopic Structures Obtained By Applying a Magnetic Field supporting
confidence: 73%
“…Due to the complex competition in energy terms in this system, there is an incomplete understanding of these structures. Similar pattern formations have been found in a multitude of systems ranging from neutron stars 2,3 to dipolar fluids 4 to vegetation patterns 5 , along with many others [6][7][8][9][10][11][12] The mixed state appears in Type-II superconductors because it is energetically favorable. In zero field, the energy gained 13 by a superconducting transition from the normal state is…”
Section: Chapter I Introductionsupporting
confidence: 58%
“…The external field decreases from h ini to 0, following Eq. (12). Once the external field becomes zero at t 0 = h ini /v, the field remains zero for t 0 ≤ t ≤ 2t 0 .…”
Section: Model and Numerical Proceduresmentioning
confidence: 95%
“…5,6,11,12,13 We consider a scalar field φ(r), where r = (x, y). The positive and negative values of φ(r) correspond to up and down spins, respectively.…”
Section: Model and Numerical Proceduresmentioning
confidence: 99%