Steady-State Hydrodynamic Lubrication Modeled With the Payvar-Salant Mass Conservation Model

被引:37
作者
Xiong, Shangwu [1 ]
Wang, Q. Jane [1 ]
机构
[1] Northwestern Univ, Dept Mech Engn, Evanston, IL 60208 USA
来源
JOURNAL OF TRIBOLOGY-TRANSACTIONS OF THE ASME | 2012年 / 134卷 / 03期
关键词
mass conservation; finite difference; hydrodynamic bearings; REYNOLDS-EQUATION; INLET SUCTION; CAVITATION; BEARINGS;
D O I
10.1115/1.4006615
中图分类号
TH [机械、仪表工业];
学科分类号
0802 ;
摘要
Steady-state smooth surface hydrodynamic lubrications of a pocketed pad bearing, an angularly grooved thrust bearing, and a plain journal bearing are simulated with the mass-conservation model proposed by Payvar and Salant. Three different finite difference schemes, i.e., the harmonic mean scheme, arithmetic mean scheme, and middle point scheme, of the interfacial diffusion coefficients for the Poiseuille terms are investigated by using a uniform and nonuniform set of meshes. The research suggests that for the problems with continuous film thickness and pressure distributions, the results obtained with these numerical schemes generally well agree with those found in the literatures. However, if the film thickness is discontinuous while the pressure is continuous, there may be an obvious deviation. Compared with both the analytical solution and other two schemes, the harmonic mean scheme may overestimate or underestimate the pressure. In order to overcome this problem artificial nodes should be inserted along the wall of the bearings where discontinuous film thickness appears. Moreover, the computation efficiency of the three solvers, i.e., the direct solver, the line-by-line the tridiagonal matrix algorithm (TDMA) solver, and the global successive over-relaxation (SOR) solver, are investigated. The results indicate that the direct solver has the best computational efficiency for a small-scale lubrication problem (around 40 thousand nodes). TDMA solver is more robust and requires the least storage, but the SOR solver may work faster than TDMA solver for thrust bearing lubrication problems. Numerical simulations of a group of grooved thrust bearings were conducted for the cases of different outer and inner radii, groove depth and width, velocity, viscosity, and reference film thickness. A curve fitting formula has been obtained from the numerical results to express the correlation of load, maximum pressure, and friction of an angularly grooved thrust bearing in lubrication. [DOI: 10.1115/1.4006615]
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页数:16
相关论文
共 41 条
[1]  
Andres L. A. S., 2006, CLASS NOTES
[2]   The finite volume solution of the Reynolds equation of lubrication with film discontinuities [J].
Arghir, M ;
Alsayed, A ;
Nicolas, D .
INTERNATIONAL JOURNAL OF MECHANICAL SCIENCES, 2002, 44 (10) :2119-2132
[3]   A Mass-Conserving Algorithm for Dynamical Lubrication Problems With Cavitation [J].
Ausas, Roberto F. ;
Jai, Mohammed ;
Buscaglia, Gustavo C. .
JOURNAL OF TRIBOLOGY-TRANSACTIONS OF THE ASME, 2009, 131 (03) :1-7
[4]   Micro-roughness effects in (elasto)hydrodynamic lubrication including a mass-flow preserving cavitation model [J].
Bayada, Guy ;
Martin, Sebastien ;
Vazquez, Carlos .
TRIBOLOGY INTERNATIONAL, 2006, 39 (12) :1707-1718
[5]   EHD ANALYSIS, INCLUDING STRUCTURAL INERTIA EFFECTS AND A MASS-CONSERVING CAVITATION MODEL [J].
BONNEAU, D ;
GUINES, D ;
FRENE, J ;
TOPLOSKY, J .
JOURNAL OF TRIBOLOGY-TRANSACTIONS OF THE ASME, 1995, 117 (03) :540-547
[6]   Cavitation formation and modelling for fluid film bearings: a review [J].
Braun, M. J. ;
Hannon, W. M. .
PROCEEDINGS OF THE INSTITUTION OF MECHANICAL ENGINEERS PART J-JOURNAL OF ENGINEERING TRIBOLOGY, 2010, 224 (J9) :839-863
[7]  
Cameron A., 1947, P I MECH ENG, V161, P59
[8]   A CAVITATION ALGORITHM [J].
ELROD, HG .
JOURNAL OF LUBRICATION TECHNOLOGY-TRANSACTIONS OF THE ASME, 1981, 103 (03) :350-354
[9]  
Elrod HG., 1974, Proceedings of the 1st Leeds-Lyon Symposium on Tribology, P37
[10]   A Modification of the Switch Function in the Elrod Cavitation Algorithm [J].
Fesanghary, M. ;
Khonsari, M. M. .
JOURNAL OF TRIBOLOGY-TRANSACTIONS OF THE ASME, 2011, 133 (02)