Oscillatory and steady shear viscosity: The Cox-Merz rule, superposition, and application to EHL friction

The new quantitative approach to elastohydrodynamic lubrication requires a description of the steady shear dependent viscosity for calculations of film thickness and friction. This property can be obtained from measurements in pressurized thin-film Couette viscometers. However, frequency dependent viscosity can be obtained from a torsionally vibrating quartz crystal viscometer at high pressure or a relatively simple ambient pressure measurement with a shear impedance spectrometer. Here it is shown for squalane and for a cyclic hydrocarbon and for a diester that both the steady shear dependent viscosity and the frequency dependent viscosity obey time-temperature-pressure superposition with the simplest shifting rule over the range of conditions investigated. Flow curves shift along a constant steady stress path or a constant complex modulus path. The Cox–Merz rule has been confirmed only for squalane and then only near the transition. The EHL friction for squalane at low pressure may be predicted with fair accuracy from the frequency dependent viscosity measured at ambient pressure. It appears that the Cox–Merz rule only applies to low-molecular-weight liquids when the molecule is composed of a long chain.

[1]  A. Dyson,et al.  Flow properties of mineral oils in elastohydrodynamic lubrication , 1965, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[2]  H. D. Cochran,et al.  Rheology of lubricant basestocks: A molecular dynamics study of C30 isomers , 2000 .

[3]  A. Wilson,et al.  Paper 3: Film Thicknesses in Elastohydrodynamic Lubrication by Silicone Fluids , 1965 .

[4]  M. Hayakawa,et al.  Electric and mechanical relaxations of LiClO4-propylene carbonate systems in 100 MHz region. , 2009, The journal of physical chemistry. B.

[5]  Scott Bair,et al.  Reference liquids for quantitative elastohydrodynamics: selection and rheological characterization , 2006 .

[6]  M. Kotzalas,et al.  The Contribution of Roller Compliance to Elastohydrodynamic Traction , 2006 .

[7]  A. J. Moore,et al.  Elastohydrodynamic lubrication at high pressures II. Non-Newtonian behaviour , 1979, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[8]  Scott Bair Shear thinning correction for rolling/sliding elastohydrodynamic film thickness , 2005 .

[9]  K. R. Harris Temperature and Pressure Dependence of the Viscosities of 2-Ethylhexyl Benzoate, Bis(2-ethylhexyl) Phthalate, 2,6,10,15,19,23-Hexamethyltetracosane (Squalane), and Diisodecyl Phthalate† , 2009 .

[10]  K. Satō,et al.  Particle-like and fluid-like settling of a stratified suspension , 2012, The European physical journal. E, Soft matter.

[11]  Wassim Habchi,et al.  Towards the true prediction of EHL friction , 2013 .

[12]  A. Dyson,et al.  Frictional traction and lubricant rheology in elastohydrodynamic lubrication , 1970, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[13]  G. J. Johnston,et al.  The elastohydrodynamic properties of some advanced non hydrocarbon-based lubricants , 1992 .

[14]  H Mizuno,et al.  Mechanical responses and stress fluctuations of a supercooled liquid in a sheared non-equilibrium state , 2012, The European physical journal. E, Soft matter.

[15]  Extension of the torsional crystal viscometer to measurements in the time domain , 2003 .

[16]  Clare McCabe,et al.  A study of mechanical shear bands in liquids at high pressure , 2004 .

[17]  Marc J. Assael,et al.  Reference Correlations for the Density and Viscosity of Squalane from 273 to 473 K at Pressures to 200 MPa , 2014 .

[18]  Hugh Spikes,et al.  Prediction of traction in elastohydrodynamic lubrication , 1998 .

[19]  S. Bair,et al.  Cavitation in creeping shear flows , 2005 .

[20]  W. Cox,et al.  Correlation of dynamic and steady flow viscosities , 1958 .

[21]  Scott Bair,et al.  High Pressure Rheology for Quantitative Elastohydrodynamics , 2007 .

[22]  S. Koda,et al.  Rheological bases for empirical rules on shear viscosity of lubrication oils. , 2013, The journal of physical chemistry. B.

[23]  W. Gleissle Two Simple Time-Shear Rate Relations Combining Viscosity and First Normal Stress Coefficient in the Linear and Non-Linear Flow Range , 1980 .

[24]  S. Bair,et al.  Fragility and the dynamic crossover in lubricants , 2007 .

[25]  Philippe Vergne,et al.  On friction regimes in quantitative elastohydrodynamics , 2013 .

[26]  P. W. Bridgman,et al.  The Viscosity of Liquids under Pressure. , 1925, Proceedings of the National Academy of Sciences of the United States of America.

[27]  V. Semjonow Drückabhängigkeit der Viskosität einiger Polyfininschmelzen , 1965 .

[28]  H. H. Winter,et al.  Viscous Dissipation in Shear Flows of Molten Polymers , 1977 .

[29]  A. Collings,et al.  Torsional crystal technique for the measurement of viscosities of liquids at high pressure , 1971 .

[30]  Philippe Vergne,et al.  A unified shear-thinning treatment of both film thickness and traction in EHD , 2005, 0704.1798.

[31]  S. Bair,et al.  A Quantitative Solution for the Full Shear-Thinning EHL Point Contact Problem Including Traction , 2007 .

[32]  Percy Williams Bridgman,et al.  The Effect of Pressure on the Viscosity of Forty-Three Pure Liquids , 1926 .

[33]  S. Bair The high pressure rheology of some simple model hydrocarbons , 2002 .

[34]  Hugh Spikes,et al.  Sixty years of EHL , 2006 .