Abstract
In this study, we propose a refined hydrodynamic lubrication model that incorporates a high-accuracy numerical algorithm for starved lubrication involving free surfaces. The performance of the proposed method is compared against that of the conventional model and numerical scheme. The results indicate that the Elrod-Adams model underestimates the hydrodynamic pressure due to unrealistic assumptions regarding the mass transport velocity of the lubricant beyond the contact region. Furthermore, the conventional numerical scheme fails to correctly predict the location of the rupture point and loses accuracy under conditions of severe starvation or high sliding speeds. In contrast, our proposed model ensures the conservation of mass flow between the outlet and inlet, while the new numerical algorithm restores the accuracy of the results.
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Data Availability
Data generated during this study are available from the corresponding authors on reasonable request.
Abbreviations
- A:
-
Location of reformation point
- B:
-
Location of rupture point
- C 1 i :
-
Coefficient
- C 2 i :
-
Coefficient
- F :
-
= θH
- G :
-
\(= - F\frac{\partial \alpha }{{\partial X}} + \frac{1}{{\Lambda }}\frac{\partial }{\partial X}\left( {H^3 \frac{\partial P}{{\partial X}}} \right)\)
- H :
-
Film thickness (m)
- h s :
-
Initial supplied film thickness (m)
- h 0 :
-
Minimum film thickness (m)
- h 1 :
-
\(= 4\delta x^2 /l^2 (m)\)
- H :
-
Dimensionless film thickness, H = h/h0
- L :
-
Length of upper surface (m)
- l c :
-
Length of calculation zone (m)
- M :
-
Mesh number
- N T :
-
Time step number
- P :
-
Pressure of fluid film (Pa)
- p a :
-
Atmospheric pressure (Pa)
- P :
-
Dimensionless fluid film pressure, P = p/pa
- Q 1 i :
-
\({{H_{i + \frac{1}{2}}^3 }}/{(\Lambda \Delta X^2) }\)
- Q 2 i :
-
\({{H_{i - \frac{1}{2}}^3 }}/{(\Lambda \Delta X^2) }\)
- Q 3 i :
-
\(= (\alpha_{i + 1}^n - \alpha_{i - 1}^n )/(2{\Delta }X)\)
- Q 4 i :
-
\(= Q_{1i} + Q_{2i}\)
- T :
-
Time (s)
- t 0 :
-
= l/u, Unit time (s)
- T :
-
= t/t0, Dimensionless time
- u :
-
Sliding speed (m/s)
- v A :
-
Velocity of reformation point (m/s)
- v B :
-
Velocity of rupture point (m/s)
- V A = :
-
vA/u, Dimensionless velocity of reformation point
- V B :
-
= vB/u, Dimensionless velocity of rupture point
- x :
-
coordinate in sliding direction
- X :
-
Dimensionless coordinate, X = x/l
- w :
-
Load-carrying capacity (N/m)
- W :
-
= w/(p0l), Dimensionless load-carrying capacity
- α :
-
Mass transport velocity
- δ :
-
Height of the upper surface (m)
- Δ t :
-
= Δx/(2u), Time step
- ΔT :
-
= Δt/t0, Dimensionless time step
- Δ x :
-
= l/m, Mesh size
- ΔX :
-
= 1/m, Dimensionless mesh size
- ε :
-
Convergence tolerance
- η :
-
Viscosity (Pa·s)
- θ :
-
Saturation variable
- ρ :
-
Cell-integrated quantity
- ρ :
-
= ∫f dx
- Ξ :
-
= -αT
- Ωf :
-
Fully filled region
- Ωp :
-
Partially filled region
- Ωt :
-
Transition region
- Λ :
-
= 12ηlu/(pAh02)
- -:
-
Left-hand limit
- + :
-
Right-hand limit
- 0:
-
Initial condition
- n :
-
Time step
- k :
-
Iteration step
- *:
-
Temporary value
- i :
-
Node index in x-direction
- Iup:
-
\(= i - sgn\left( {\alpha_i } \right)\)
- Icell:
-
= i—½
- A :
-
Reformation point
- B :
-
Rupture point
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The funding was provided by the Research Committee RC282 of the Japan Society of Mechanical Engineers.
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K.Y. formulated the research concept and supervised the study. K.Z. developed the software for conducting the numerical simulation. K.Z. and K.Y. prepared the manuscript, including the texts, figures, and tables. K.Z. and K.Y. contributed to and approved the discussion of the results.
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Zhang, K., Yagi, K. Refined Hydrodynamic Lubrication Model with a High-Accuracy Numerical Algorithm for Starved Lubrication with Free Surfaces. Tribol Lett 71, 122 (2023). https://doi.org/10.1007/s11249-023-01789-2
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DOI: https://doi.org/10.1007/s11249-023-01789-2