Abstract
Based on the Shliomis model for ferrofluid flow and continuity equation, modified Reynolds equation for the study of lubrication of different slider bearings, is derived by considering the effects of oblique radially variable magnetic field and squeeze velocity. The Shliomis model is important because it includes the effects of rotations of the carrier liquid as well as magnetic particles. The variable magnetic field is important because of its advantage of generating maximum field at the required active contact zone. Using Reynolds equation, expressions for dimensionless load-carrying capacity, frictional force, coefficient of friction and center of pressure are obtained. Using these expressions, results for different slider bearings are computed for different parameters and compared.
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Abbreviations
- a :
-
\( \frac{{h_{2} }}{{h_{1} }} \)
- A :
-
Bearing length (m)
- B :
-
Bearing breadth (m)
- f :
-
Coefficient of friction
- \( \bar{f} \) :
-
Dimensionless coefficient of friction defined in Eq. (29)
- F :
-
Frictional force on the slider (N)
- \( \bar{F} \) :
-
Dimensionless frictional force defined in Eq. (28)
- h :
-
Film thickness (m)
- \( \bar{h} \) :
-
Dimensionless quantity defined in Eq. (21)
- \( h_{1} ,h_{2} \) :
-
Minimum and maximum values of h (m)
- \( \dot{h}_{1} \) :
-
Squeeze velocity, \( \frac{{dh_{1} }}{dt}\;({\text{m}}\;{\text{s}}^{ - 1} ) \)
- H :
-
Magnetic field strength (A m−1)
- H :
-
Magnetic field vector
- I :
-
Sum of moments of inertia of the particles per unit volume (N s2 m−2)
- \( I^{*} ,I^{**} \) :
- K :
-
Quantity defined in Eq. (12) (A m−3)
- \( k_{B} \) :
-
Boltzmann constant (J(°K)−1)
- m :
-
Magnetic moment of a particle (A m2)
- M :
-
Magnetization vector
- \( M_{0} \) :
-
Saturation magnetization (A m−1)
- n :
-
Number of particles per unit volume (m−3)
- p :
-
Film pressure (N m−2)
- \( \bar{p} \) :
-
Dimensionless film pressure defined in Eq. (21)
- q = (u, 0, w):
-
Fluid velocity vector
- t :
-
Time (s)
- T :
-
Temperature (°K)
- U :
-
Slider velocity (ms−1)
- W :
-
Load-carrying capacity (N)
- \( \bar{W} \) :
-
Dimensionless load-carrying capacity defined Eq. (27)
- x,y,z :
-
Coordinates
- \( \bar{x} \) :
-
x-Coordinates of the center of pressure (m)
- \( \bar{\bar{x}} \) :
-
Dimensionless center of pressure defined in Eq. (30)
- X :
-
\( \frac{x}{A} \)
- \( \upalpha \) :
-
Inclination of the magnetic field with the x-axis
- \( \upbeta \) :
-
Squeeze velocity parameter defined in Eq. (21)
- \( \updelta \) :
-
Central thickness of the convex pad (m)
- \( \bar{\updelta } \) :
-
\( \frac{\updelta }{{h_{1} }} \)
- \( \upeta \) :
-
Viscosity of the suspension (N s m−2)
- \( \upeta_{0} \) :
-
Viscosity of the liquid carrier (N s m−2)
- \( \uplambda \) :
-
Magnetic field strength parameter defined in Eq. (23)
- \( \upmu_{0} \) :
-
Permeability of free space
- \( \upxi \) :
-
Dimensionless field strength (Langevin’s parameter)
- \( \uptau \) :
-
Rotational viscosity parameter
- \( \bar{\uptau } \) :
-
Defined in Eq. (10)
- \( \uptau_{B} \) :
-
Brownian relaxation time (s)
- \( \uptau_{s} \) :
-
Magnetic moment relaxation time (s)
- \( \bar{\Omega } \) :
-
\( \tfrac{1}{2}\nabla \times \;{\mathbf{q}} \)
- ϕ:
-
Volume concentration of the particles
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The authors are thankful to the Reviewer, Associate Editor and Editor in Chief for their valuable comments.
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Shah, R.C., Shah, R.B. Derivation of ferrofluid lubrication equation for slider bearings with variable magnetic field and rotations of the carrier liquid as well as magnetic particles. Meccanica 53, 857–869 (2018). https://doi.org/10.1007/s11012-017-0788-9
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DOI: https://doi.org/10.1007/s11012-017-0788-9