2009
DOI: 10.1134/s1063776109050173
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Regular and chaotic dynamics of a chain of magnetic dipoles with moments of inertia

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Cited by 20 publications
(4 citation statements)
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“…The bodies with dipole moments are considered to be homogeneous and spherical [7]. The dynamic equa tions for the system of dipoles have the following form [8][9][10]: (1) where and are the dipole moment and the angular velocity of the ith dipole ( is the angle of rotation of the ith dipole about the axis j = x, y, z of the Cartesian system of coordinates); J i is the moment of inertia; and α i is the dissipation parameter. In the absence of an external field, the field that is created at…”
Section: Initial Equationsmentioning
confidence: 99%
See 1 more Smart Citation
“…The bodies with dipole moments are considered to be homogeneous and spherical [7]. The dynamic equa tions for the system of dipoles have the following form [8][9][10]: (1) where and are the dipole moment and the angular velocity of the ith dipole ( is the angle of rotation of the ith dipole about the axis j = x, y, z of the Cartesian system of coordinates); J i is the moment of inertia; and α i is the dissipation parameter. In the absence of an external field, the field that is created at…”
Section: Initial Equationsmentioning
confidence: 99%
“…If an external field f is applied, it is added to the field (2). The dipoles that make up the lattice are assumed to be identical, i.e., and Let us now pass to the following dimensionless parameters [8,9]:…”
Section: A M Shutyimentioning
confidence: 99%
“…In biological environments, magnetic particles in bacteria can affect the movements of these bacteria in a changing external magnetic field [5]. Theoretical calculations have already shown that the rotation of linearly connected magnetic dipoles (magnetic chains) can show chaotic behaviour in sinusoid alternating external fields [6], while other results have suggested a phenomenon of synchronization [7].…”
Section: Introductionmentioning
confidence: 99%
“…Each nanoparticle can rotate about the center of masses. The dynamic equations for this system of magnetic dipoles can be represented as follows [9][10][11]: (1) where and are the dipole magnetic moment and the angular velocity of the ith dipole (ϕ ij is the angle of rotation of the dipole about the axis ), is the moment of inertia, and is the dissipation parameter. The effective field produced at the site of the location of the ith dipole by the other dipoles and by an external magnetic field h is deter mined as follows:…”
Section: Introductionmentioning
confidence: 99%