2012
DOI: 10.1016/j.expthermflusci.2012.01.003
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Motion of a deformable drop of magnetic fluid on a solid surface in a rotating magnetic field

Abstract: 9 pages, 4 figuresInternational audienceThe behavior of a magnetic fluid drop lying on a solid horizontal surface and surrounded by a nonmagnetic liquid under the action of a uniform magnetic field which is rotating in a vertical plane with low frequency (of the order of 1 Hz) has been investigated experimentally. Shape deformation and translatory motion of the drop were observed and studied. The drop translation velocity for different field amplitudes and field frequencies has been measured

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Cited by 38 publications
(23 citation statements)
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“…When subjected to a rotating magnetic field circularly polarized in the ( x , z ) plane H ( t ) = H 0 (cos (2 πft ) e x − sin (2 πft ) e z ), the LRM tends to spin to follow the field because the rotating magnetic field generates torques on the suspended magnetic nanoparticles in the ferrofluid, together with the viscous coupling between the particles and the surrounding carriers cause the droplet to follow externally rotate H . [ 35 ] If closed to the substrate, the rotating LRM will become a surface walker, as shown in Figure 2d. Usually, because the Reynolds coefficient (Re) is much smaller than 1, which is about 10 −3 or less at the micrometer scale, the inertial force of the LRM can be neglected, and its kinematic equation degenerates into a first‐order model.…”
Section: Resultsmentioning
confidence: 99%
“…When subjected to a rotating magnetic field circularly polarized in the ( x , z ) plane H ( t ) = H 0 (cos (2 πft ) e x − sin (2 πft ) e z ), the LRM tends to spin to follow the field because the rotating magnetic field generates torques on the suspended magnetic nanoparticles in the ferrofluid, together with the viscous coupling between the particles and the surrounding carriers cause the droplet to follow externally rotate H . [ 35 ] If closed to the substrate, the rotating LRM will become a surface walker, as shown in Figure 2d. Usually, because the Reynolds coefficient (Re) is much smaller than 1, which is about 10 −3 or less at the micrometer scale, the inertial force of the LRM can be neglected, and its kinematic equation degenerates into a first‐order model.…”
Section: Resultsmentioning
confidence: 99%
“…For frequencies up to 40 Hz, an s-shape, or spiral, formation of the ferrofluid has also been investigated [12,13].…”
Section: Introductionmentioning
confidence: 99%
“…e basis for the construction of an RMF was taken from [13] and [15][16][17] and modified in such a way that magnetic fields could be generated suitable for medical hyperthermia.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, they offer a broad range of application prospectives such as in medicine [11][12][13] and technology [14][15][16][17]. However, whereas such ferrofluids, i.e., colloidal suspensions of magnetic particles in isotropic liquids, display fascinating behaviors in the presence of an external magnetic field, actual systems exhibit only zero net magnetization once the external field is switched off, i.e., there is no occurrence of spontaneous symmetry breaking [18][19][20][21].…”
Section: Introductionmentioning
confidence: 99%