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Ferrofluids are industrially prepared fluids which consist of highly concentrated, stable colloidal suspensions of fine magnetic particles in a suitable fluid carrier (water, kerosine, diester, etc.). these are, essentially, nonconducting substances which globally present a temperature–dependent magnetization at a constant applied magnetic fields. they exhibit a nonlinear magnetic behavior, with a saturation effect, for sufficiently strong applied magnetic fields.

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Notes

  1. Medvedev and Krakov [1983] and Zimmels [1983].

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  2. Jenkins [1972] has derived (12.2.16) by using a different thermodynamical approach. The present derivation follows Maugin [1978c], see also [1974c] for relativistic spinning fluids.

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  3. See Maugin [1978i] and Maugin and Drouot [1983].

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  4. We follow Brancher [1980a].

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  5. Equation (12.5.10) was first derived by Neuringer and Rosenweig [1964] by means of a classical thermodynamical approach different from the one given here. For some early discussions of ferrofluids, see Rosensweig [1966], [1970].

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  6. Compare (12.6.4) and (11.5.2).

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  7. Compare (12.6.9) and (11.5.6).

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  8. Neuringer and Rosenweig [1964].

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  9. Neuringer and Rosenweig (1964).

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  10. See Resler and Neuringer [1964].

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  11. Neuringer and Rosensweig [1964].

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  12. See Whittaker and Watson [1946, p. 373].

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  13. Neuringer [1966].

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  14. Neuringer [1966].

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  15. See Eringen [1980, p. 276].

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  16. This can also be derived in ferrofluids by accounting for density gradients in the constitutive theory (see Maugin [1978i]).

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© 1990 Springer-Verlag New York Inc.

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Eringen, A.C., Maugin, G.A. (1990). Ferrofluids. In: Electrodynamics of Continua II. Springer, New York, NY. https://doi.org/10.1007/978-1-4612-3236-0_4

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  • DOI: https://doi.org/10.1007/978-1-4612-3236-0_4

  • Publisher Name: Springer, New York, NY

  • Print ISBN: 978-1-4612-7928-0

  • Online ISBN: 978-1-4612-3236-0

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