Bénard–Marangoni ferroconvection with magnetic field dependent viscosity
The effect of magnetic field dependent viscosity on the onset of Bénard–Marangoni ferroconvection in a horizontal layer of ferrofluid is investigated theoretically. The lower boundary is taken to be rigid with fixed temperature, while the upper free boundary at which temperature-dependent surface te...
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Published in | Journal of magnetism and magnetic materials Vol. 322; no. 15; pp. 2256 - 2263 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Amsterdam
Elsevier B.V
01.08.2010
Elsevier |
Subjects | |
Online Access | Get full text |
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Summary: | The effect of magnetic field dependent viscosity on the onset of Bénard–Marangoni ferroconvection in a horizontal layer of ferrofluid is investigated theoretically. The lower boundary is taken to be rigid with fixed temperature, while the upper free boundary at which temperature-dependent surface tension effect is considered is non-deformable and subject to a general thermal condition. The Rayleigh–Ritz method with Chebyshev polynomials of the second kind as trial functions is employed to extract the critical stability parameters numerically. The results show that the onset of ferroconvection is delayed with an increase in the magnetic field dependent viscosity parameter (
Λ) and Biot number (
Bi) but opposite is the case with an increase in the value of magnetic Rayleigh number (
R
m
) and nonlinearity of magnetization (
M
3). Further, increase in
R
m
,
M
3, and decrease in
Λ and
Bi is to decrease the size of the convection cells. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 ObjectType-Article-2 ObjectType-Feature-1 |
ISSN: | 0304-8853 |
DOI: | 10.1016/j.jmmm.2010.02.021 |