2007
DOI: 10.1103/physreve.75.061405
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Magnetic properties of polydisperse ferrofluids: A critical comparison between experiment, theory, and computer simulation

Abstract: Experimental magnetization curves for a polydisperse ferrofluid at various concentrations are examined using analytical theories and computer simulations with the aim of establishing a robust method for obtaining the magnetic-core diameter distribution function p(x). Theoretical expressions are fitted to the experimental data to yield the parameters of p(x). It is shown that the majority of available theories yield results that depend strongly on the ferrofluid concentration, even though the magnetic compositi… Show more

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Cited by 141 publications
(157 citation statements)
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References 29 publications
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“…For example, the magnetization curves for a highly polydisperse magnetite ferrofluid were reproduced essentially exactly by a modified mean-field model and computer simulations of a polydisperse DHS fluid. 37,38 The paper is organized as follows. Section II contains a definition of the DHS model, the interaction potentials, and the thermodynamic parameters.…”
Section: Introductionmentioning
confidence: 99%
“…For example, the magnetization curves for a highly polydisperse magnetite ferrofluid were reproduced essentially exactly by a modified mean-field model and computer simulations of a polydisperse DHS fluid. 37,38 The paper is organized as follows. Section II contains a definition of the DHS model, the interaction potentials, and the thermodynamic parameters.…”
Section: Introductionmentioning
confidence: 99%
“…At intermediate values, the magnetic saturation for noninteracting permanent dipoles is predicted by Langevin theory [14] as a function of α B = mB/k B T . A recent study of ferrofluids in a uniform field [26] has shown that the noninteracting Langevin theory is still applicable in systems with moderate dipole-dipole interactions. Figure 3 shows domain morphology snapshots for simulations in which the quench was made with a uniform magnetic field present from the outset, with α B = 2 and 20 respectively and with λ = 4.…”
Section: Effect Of Uniform External Fieldmentioning
confidence: 99%
“…The finite element (FE) mesh required for the segmented brain was generated using Computer Geometry Algorithm Library (CGAL) according to previously described method (Lee et al, 2012). The relative magnetization, M rel , defined as the ratio M/M S , where M S is the saturation magnetization, was computed using standard magnetic dynamic formalism described elsewhere (Ivanov et al, 2007;Mikhaylova et al, 2004). The effect of the local electric field was modeled through the local point magnetization change according to the aforementioned linear expression for the ME effect.…”
Section: Methodsmentioning
confidence: 99%