Modelling and full-scale trials to investigate fluid pressurisation of rolling contact fatigue cracks

Abstract Fluid penetration of cracks has been regarded as an important mechanism of crack growth for inclined surface breaking cracks under contact loading since the 1930s. However, there are only limited cases in which it is realistic to assume fluid is sealed in and pressurised by wheels crossing cracks of complex three-dimensional morphology in rolling contact fatigue affected rail. To investigate, modelling to predict crack growth rates was conducted following experimental verification that fluid penetration occurs for a full size rail-wheel contact. A fluid filled crack beneath a three-dimensional elliptic contact was modelled through development of an existing two-dimensional model. Stress intensity factor results from this model were in good agreement with available literature values, indicating very high growth rates for cracks containing pressurised fluid. At larger crack sizes, for which it was assumed the contact could not seal fluid inside the crack, a shear mode crack growth model was applied. This predicted much lower crack growth rates, of around ten times the rail wear rate, indicating a crack growing sufficiently fast to “keep ahead” of wear, but not unrealistically fast. Further work to correlate the predictions of the fluid pressurisation model with field measurements was suggested.

[1]  Y. Murakami Stress Intensity Factors Handbook , 2006 .

[2]  John H. Beynon,et al.  A simple method of stress intensity factor calculation for inclined fluid-filled surface-breaking cracks under contact loading , 1999 .

[3]  Yukitaka Murakami,et al.  Mechanism of Surface Crack Growth in Lubricated Rolling/Sliding Spherical Contact , 1986 .

[4]  D. P. Rooke,et al.  Crack-line and edge Green's functions for stress intensity factors of inclined edge cracks , 1991 .

[5]  Ajay Kapoor,et al.  Investigating fluid penetration of rolling contact fatigue cracks in rails using a newly developed full-scale test facility , 2007 .

[6]  Stanisław Bogdański A rolling contact fatigue crack driven by squeeze fluid film , 2002 .

[7]  A. Bower The influence of crack face friction and trapped fluid on surface initiated rolling contact fatigue cracks , 1988 .

[8]  John H. Beynon,et al.  Development of a machine for closely controlled rolling contact fatigue and wear testing , 2000 .

[9]  K. Johnson,et al.  Plastic flow and shakedown of the rail surface in repeated wheel-rail contact , 1991 .

[10]  Makoto Akama Fatigue Crack Growth under Mixed Loading of Tensile and In-plane Shear Modes , 2003 .

[11]  Ajay Kapoor,et al.  Rapid method of stress intensity factor calculation for semi-elliptical surface breaking cracks under three-dimensional contact loading , 2006 .

[12]  Y. J. Huang,et al.  Prediction of the fatigue threshold for a cracked body using shakedown theory , 1995 .

[13]  John H. Beynon,et al.  A simple method of stress intensity factor calculation for inclined surface-breaking cracks with crack face friction under contact loading , 1999 .

[14]  M. W. Brown,et al.  Shear mode crack growth and rolling contact fatigue , 1991 .

[15]  M. N. Webster,et al.  An Experimental Investigation of Micropitting Using a Roller Disk Machine , 1995 .

[16]  R. J. Crawford,et al.  Mechanics of engineering materials , 1986 .