Abstract
In this work, we present a theoretical study on the stability of a two-dimensional plane Poiseuille flow of magnetic fluids in the presence of externally applied magnetic fields. The fluids are assumed to be incompressible, and their magnetization is coupled to the flow through a simple phenomenological equation. Dimensionless parameters are defined, and the equations are perturbed around the base state. The eigenvalues of the linearized system are computed using a finite difference scheme and studied with respect to the dimensionless parameters of the problem. We examine the cases of both the horizontal and vertical magnetic fields. The obtained results indicate that the flow is destabilized in the horizontally applied magnetic field, but stabilized in the vertically applied field. We characterize the stability of the flow by computing the stability diagrams in terms of the dimensionless parameters and determine the variation in the critical Reynolds number in terms of the magnetic parameters. Furthermore, we show that the superparamagnetic limit, in which the magnetization of the fluids decouples from hydrodynamics, recovers the same purely hydrodynamic critical Reynolds number, regardless of the applied field direction and of the values of the other dimensionless magnetic parameters.
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Abbreviations
- B :
-
magnetic induction field (T)
- H :
-
applied magnetic field (A/m)
- H 0 :
-
magnetic field intensity (A/m)
- ℓ :
-
half distance between plates (m)
- M :
-
magnetization of magnetic fluid (A/m)
- M 0 :
-
equilibrium magnetization of magnetic fluid (A/m)
- p :
-
pressure (Pa)
- u :
-
velocity field (m/s)
- U :
-
characteristic velocity scale (m/s)
- η :
-
dynamic viscosity of fluid (Pa·s)
- μ 0 :
-
vacuum magnetic permeability (H/m)
- ρ :
-
fluid density (kg/m3)
- σ :
-
stress tensor of magnetic fluid (Pa)
- τ :
-
magnetic relaxation time (s)
- \({\cal A},{\cal B}\) :
-
functions appearing on perturbed magnetization equations
- B :
-
magnetic induction
- c :
-
propagation velocity of perturbation
- c i :
-
imaginary part of propagation velocity of perturbation
- c r :
-
real part of propagation velocity of perturbation
- e x :
-
unit vector on horizontal direction
- H :
-
magnetic field
- i:
-
imaginary unity, \({\rm{i}} = \sqrt {- 1} \)
- j :
-
index of mesh points
- M :
-
magnetization of magnetic fluid
- n :
-
unitary normal vector
- N :
-
number of mesh points
- P :
-
block matrix appearing in generalized eigenvalue problem
- Q :
-
block matrix appearing in generalized eigenvalue problem
- u :
-
horizontal velocity component
- \({\tilde w}\) :
-
combined vector of amplitudes for generalized eigenvalue problem
- α :
-
wave number of perturbation
- Δy :
-
mesh size
- ϵ :
-
Levi-Civita permutation tensor
- C pm :
-
magnetic pressure coefficient, \({C_{pm}} = {{{\mu _0}H_0^2} \over {\rho {U^2}}}\)
- Pe :
-
Péclet number, \(Pe = {{\tau U} \over \ell}\)
- Re :
-
Reynolds number, \(Re = {{\rho U\ell} \over \eta}\)
- Re c :
-
critical Reynolds number
- Re hc :
-
critical Reynolds number for purely hydrodynamical problem
- γ :
-
exponent of power law relation between Rec and Cpm
- χ0:
-
magnetic susceptibility
- {·}b :
-
base state variables
- {·}1 :
-
horizontal component of vector
- {·}2 :
-
vertical component of vector
- \(\widetilde{\left\{\cdot \right\}}\) :
-
amplitudes of perturbations
- {·}′:
-
perturbations of variables
- \({{\cal L}_{{\rm{OS}}}}\) :
-
Orr-Sommerfeld operator.
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Acknowledgements
P. Z. S. PAZ is grateful for the financial support provided by Coordination for the Improvement of Higher Education Personnel-Brazil (CAPES) (Finance Code 001) and National Council for Scientific and Technological Development-Brazil (CNPq) during the course of this research. F. R. CUNHA acknowledges the financial support of CNPq (No. 305764/2015-2). Y. D. SOBRAL acknowledges the financial support of University of Brasilia (Call DPI/DPG No. 02/2021).
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Paz, P.Z.S., Cunha, F.R. & Sobral, Y.D. Stability of plane-parallel flow of magnetic fluids under external magnetic fields. Appl. Math. Mech.-Engl. Ed. 43, 295–310 (2022). https://doi.org/10.1007/s10483-022-2813-9
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DOI: https://doi.org/10.1007/s10483-022-2813-9