Effect of Inlet Shear Heating Due to Sliding on Elastohydrodynamic Film Thickness

1983 ◽  
Vol 105 (2) ◽  
pp. 187-188 ◽  
Author(s):  
W. R. D. Wilson ◽  
S. Sheu
1981 ◽  
Vol 103 (2) ◽  
pp. 295-301 ◽  
Author(s):  
J. J. Coy ◽  
E. V. Zaretsky

Elastohydrodynamic film thickness was measured for a 20-mm ball bearing using the capacitance technique. The bearing was thrust loaded to 90, 448, and 778 N (20, 100, and 175 lb). The corresponding maximum stresses on the inner race were 1.28, 2.09, and 2.45 GPa (185,000, 303,000, and 356,000 psi). Test speeds ranged from 400 to 14,000 rpm. Film thickness measurements were taken with four different lubricants: (a) synthetic paraffinic, (b) synthetic paraffinic with additives, (c) neopentylpolyol (tetra) ester meeting MIL-L-23699A specifications, and (d) synthetic cycloaliphatic hydrocarbon traction fluid. The test bearing was mist lubricated. Test temperatures were 300, 338, and 393 K. The measured results were compared to theoretical predictions using the formulae of Grubin, Archard and Cowking, Dowson and Higginson, and Hamrock and Dowson. There was good agreement with theory at low dimensionless speed, but the film was much smaller than theory predicts at higher speeds. This was due to kinematic starvation and inlet shear heating effects. Comparisons with Chiu’s theory on starvation and Cheng’s theory on inlet shear heating were made.


Author(s):  
D. A. Jones ◽  
A. B. Crease

This paper describes an attempt to measure the elastohydrodynamic film thickness generated within the rolling contacts of a conventional taper roller thrust bearing. The technique used is simple and unambiguous and should be capable of application irrespective of the surface finish or geometry of the rolling elements.


2010 ◽  
Vol 132 (2) ◽  
Author(s):  
H. Dormois ◽  
N. Fillot ◽  
W. Habchi ◽  
G. Dalmaz ◽  
P. Vergne ◽  
...  

This paper presents a study of the spinning influence on film thickness and friction in EHL circular contacts under isothermal and fully flooded conditions. Pressure and film thickness profiles are computed with an original full-system finite element approach. Friction was thereafter investigated with the help of a classical Ree–Eyring model to calculate the longitudinal and transverse shear stresses. An analysis of both the velocity and shear stress distributions at every point of the contact surfaces has allowed explaining the fall of the longitudinal friction coefficient due to the occurrence of opposite shear stresses over the contact area. Moreover in the transverse direction spinning favors large shear stresses of opposite signs, decreasing the fluid viscosity by non-Newtonian effects. These effects have direct and coupled consequences on the friction reduction that is observed in the presence of spinning. They are expected to further decrease friction in real situations due to shear heating.


2013 ◽  
Vol 64 ◽  
pp. 33-38 ◽  
Author(s):  
Scott Bair ◽  
Ivan Krupka ◽  
Petr Sperka ◽  
Martin Hartl

2004 ◽  
Vol 47 (1) ◽  
pp. 123-129 ◽  
Author(s):  
HAIXIA YANG ◽  
STEVEN R. SCHMID ◽  
THOMAS J. KASUN ◽  
RONALD A. REICH

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