Elastohydrodynamic lubrication at high pressures

Film thickness and traction have been measured in a two-disk machine over a range of rolling and sliding speeds, by using two mineral oils which have previously been studied at lower pressures. The results show: (1) That the lubricant film thickness is correctly given by ‘classical’ elastohydrodynamic theory, even when the behaviour of the lubricant in the high pressure regions is quite different from the Newtonian viscous behaviour postulated in the theory. (2) That over the range of pressure 0.7-2.5GPa both oils behave as elastic solids with a well defined shear modulus. (3) That the elastic compliance of the disks may be comparable with or exceed that in the oil film and must be taken into account in the calculation of the shear modulus of the oils. (4) That at these high pressures the elastic properties, not the viscous properties, of the oil determine the traction when the shear is small. (5) That there is an elastic limit at a critical shear stress above which the shear increases more rapidly than the stress. The magnitude of this critical stress increases with the pressure. (6) That the transition from viscous to elastic behaviour takes place over a relatively narrow range of pressure above which the elastic behaviour becomes insensitive to the rolling speed at which the tests are performed.

It was shown in two earlier papers that the behaviour of many mineral oils and silicone fluids in impact agrees with theory when the effects of temperature are properly taken into account. The behaviour of some fluids of high viscosity could not be explained and these fluids appeared to possess elastic properties. It is shown that the effects observed earlier can be reproduced using polymer solutions. By varying the strength of the solution and the initial film thickness a range of effects can be seen and the observed phenomena comprise a systematic pattern. It has been found that under all but the most extreme conditions the elastic behaviour is the result of the compression of the film; elastic behaviour in shear is seldom observed. Elastic effects are exhibited by all fluids in the appropriate conditions and criteria are given for the detection of both shear and compressive elastic effects in the presence of viscous flow. The theory of the impact of compressible fluids has been developed and shown to agree with experiment. It explains the behaviour of the fluids which had previously been thought to be anomalous. In addition, it predicts that the pressure distribution differs greatly from that in viscous conditions and changes with time. This prediction has been confirmed by direct experimental measurement.


The paper describes measurements of the film thickness and traction given in elastohydrodynamic lubrication by polyphenyl ether. The film thickness is well below the theoretical value and very sensitive to temperature but its variation with load is of the theoretical magnitude. The tractional behaviour is more complex than that of mineral oils and this is thought to be due to the variation of the pressure distribution with speed and load. The results indicate that the fluid behaves elastically when the slip is small, even at the lowest load. Above a critical stress the relation between the shear stress and the rate of shear becomes non-linear. The non-Newtonian characteristics of this ’elastic’ fluid then become similar to those of a ‘viscous’ fluid.


1977 ◽  
Vol 99 (2) ◽  
pp. 264-275 ◽  
Author(s):  
B. J. Hamrock ◽  
D. Dowson

Utilizing the theory developed by the authors in an earlier publication, the influence of the ellipticity parameter, the dimensionless speed, load, and material parameters on minimum film thickness was investigated. The ellipticity parameter was varied from one (a ball on a plate configuration) to eight (a configuration approaching a line contact). The dimensionless speed parameter was varied over a range of nearly two orders of magnitude. The dimensionless load parameter was varied over a range of one order of magnitude. Conditions corresponding to the use of solid materials of bronze, steel, and silicon nitride and lubricants of paraffinic and naphthenic mineral oils were considered in obtaining the exponent in the dimensionless material parameter. Thirty-four different cases were used in obtaining the minimum film thickness formula given below as H¯min=3.63U0.68G0.49W−0.073(1−e−0.68k) A simplified expression for the ellipticity parameter was found where k=1.03RyRx0.64 Contour plots were also shown which indicate in detail the pressure spike and two side lobes in which the minimum film thickness occurs. These theoretical solutions of film thickness have all the essential features of the previously reported experimental observations based upon optical interferometry.


1969 ◽  
Vol 91 (3) ◽  
pp. 464-475 ◽  
Author(s):  
P. E. Fowles

Conventional elastohydrodynamic theory is modified and applied to the collision between two idealized surface asperities in an isothermal sliding system. Solutions for the pressure and film thickness between the asperities as functions of their overlap, the sliding speed, the pressure-viscosity coefficient of the lubricant, and the time since the initiation of the collision are obtained numerically for the first half of the collision process. It is shown that extremely high pressures and small film thicknesses are to be expected at the center of the contact region assuming the rheology of the lubricant film can be represented by that of the bulk lubricant.


1976 ◽  
Vol 98 (3) ◽  
pp. 367-372 ◽  
Author(s):  
P. K. Gupta

An inlet zone analysis is presented for the elastohydrodynamic lubrication of heavily loaded contacts of layered elastic solids under isothermal and isoviscous conditions. An elastic layer of incompressible elastomeric material (with Poisson’s ratio, ν = 0.50) bonded to a rigid substrate is considered. Numerical results are presented in dimensionless form to describe the variation of nominal film thickness over a wide range of loads, layer thicknesses, and other operating variables.


Author(s):  
B K Karthikeyan ◽  
M Teodorescu ◽  
H Rahnejat ◽  
S J Rothberg

Isothermal and thermoelastohydrodynamic lubrication (TEHL) analyses of grease lubricated bearings are presented. A grease plug flow is formed in the conjunction that, with no shear at the boundaries with the solid surfaces, adheres to them in the region of high pressures under isothermal conditions. The elastohydrodynamic lubrication grease pressure distribution conforms fairly closely to that of its base oil alone, with the exception of inlet trail and pressure spike regions. The dependency of film thickness on speed (rolling viscosity) and load parameters for the base oil agrees with previously reported findings of the research community. For grease there are subtle differences with the base oil film thickness load and speed dependencies. However, it is clear that extrapolated oil film thickness formulae for oils can be used reasonably for the prediction of grease films, at least as a first approximation. The results presented agree well with optical interferometric measurements reported in the literature for grease-lubricated contacts at low temperatures and low surface velocities. TEHL analysis shows breakdown of the plug flow and significant reduction in film thickness, which can lead to changes in the regime of lubrication to mixed or boundary conditions.


Author(s):  
T.E. Pratt ◽  
R.W. Vook

(111) oriented thin monocrystalline Ni films have been prepared by vacuum evaporation and examined by transmission electron microscopy and electron diffraction. In high vacuum, at room temperature, a layer of NaCl was first evaporated onto a freshly air-cleaved muscovite substrate clamped to a copper block with attached heater and thermocouple. Then, at various substrate temperatures, with other parameters held within a narrow range, Ni was evaporated from a tungsten filament. It had been shown previously that similar procedures would yield monocrystalline films of CU, Ag, and Au.For the films examined with respect to temperature dependent effects, typical deposition parameters were: Ni film thickness, 500-800 A; Ni deposition rate, 10 A/sec.; residual pressure, 10-6 torr; NaCl film thickness, 250 A; and NaCl deposition rate, 10 A/sec. Some additional evaporations involved higher deposition rates and lower film thicknesses.Monocrystalline films were obtained with substrate temperatures above 500° C. Below 450° C, the films were polycrystalline with a strong (111) preferred orientation.


2013 ◽  
Vol 420 ◽  
pp. 30-35
Author(s):  
Khanittha Wongseedakaew ◽  
Jesda Panichakorn

This paper presents the effects of rough surface air-soft elastohydrodynamic lubrication (EHL) of rollers for soft material under the effect of air molecular slip. The time independent modified Reynolds equation and elasticity equation were solved numerically using finite different method, Newton-Raphson method and multigrid multilevel methods were used to obtain the film pressure profiles and film thickness in the contact region. The effects of amplitude of surface roughness, modulus of elasticity and air inlet temperature are examined. The simulation results showed surface roughness has effect on film thickness but it little effect to air film pressure. When the amplitude of surface roughness and modulus of elasticity increased, the air film thickness decreased but air film pressure increased. However, the air inlet temperature increased when the air film thickness increased.


2015 ◽  
Vol 138 (2) ◽  
Author(s):  
W. Wu ◽  
J. Wang ◽  
C. H. Venner

A high-order polynomial gas distribution cam mechanism is investigated theoretically from the viewpoint of thermal elastohydrodynamic lubrication (EHL). First, a cam with a larger base circle radius is employed, which results in slide–roll ratio 2.0 < S < 9.0 when the two surfaces move oppositely. The pressure, film thickness, and temperature profiles at a number of angular positions of the cam are presented, together with the isothermal results. The comparison between thermal and isothermal oil characteristics is also shown. It is revealed that the isothermal analysis partly overestimates the actual film thickness and it also misses some essential local phenomena. Second, a cam with a smaller base circle radius is studied, which leads to drastic variations in the slide–roll ratio which encounters four times’ occurrences of infinity in one working period. The pressure, film thickness, and temperature profiles at some angular cam positions together with the oil characteristics are given, showing much dramatic variations. A very small film thickness is observed at the contact of the tappet with the start of the cam basic segment, which suggests a possible risk of direct contact of both surfaces.


Author(s):  
Eduardo de la Guerra Ochoa ◽  
Javier Echávarri Otero ◽  
Enrique Chacón Tanarro ◽  
Benito del Río López

This article presents a thermal resistances-based approach for solving the thermal-elastohydrodynamic lubrication problem in point contact, taking the lubricant rheology into account. The friction coefficient in the contact is estimated, along with the distribution of both film thickness and temperature. A commercial tribometer is used in order to measure the friction coefficient at a ball-on-disc point contact lubricated with a polyalphaolefin base. These data and other experimental results available in the bibliography are compared to those obtained by using the proposed methodology, and thermal effects are analysed. The new approach shows good accuracy for predicting the friction coefficient and requires less computational cost than full thermal-elastohydrodynamic simulations.


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