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Reconstruction and Fundamental Explanation of the Whole Life Rail Model

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Reconstruction and Fundamental Explanation of the Whole Life Rail Model

A.A. Meghoe, R. Loendersloot , T. Tinga

University of Twente

Department of Mechanics and Solids Surfaces and Systems Section of Dynamics Based Maintenance

Introduction

Rail infrastructure managers are in constant search of reliable wear and Rolling Contact Fatigue (RCF) damage prediction models. The Whole Life Rail Model (WLRM), shown in Figure 1, is such an example.

Limitations of WLRM: - Empirically determined - Material (rail) dependent

- Only applicable to certain conditions Solution

Application of physical knowledge and fundamental analyses to construct WLRM for various materials and operating conditions.

Figure 3 shows that by using the semi-analytical solutions for 𝑁𝑖 and 𝑁𝑝 the first part of the WLRM is successfully

reconstructed. It can be seen that the WLRM depends on the coefficient of friction (cof) as the offset of the fatigue threshold shift for different cof. Current research focusses on the reconstruction of the second part of the WLRM.

PhD progress 1 2 3 4

Results

Approach

The Fatigue threshold and RCF only part of WLRM (Figure 1) can be reconstructed by taking into account the number of cycles to crack initiation (𝑁𝑖) and crack propagation (𝑁𝑝)

as calculated by (Li et al. 2017):

References

[1] Burstow, M. C. 2006. 'A Model to Predict and

Understand Rolling Contact Fatigue in Wheels and Rails'. [2] Li, C., W. Dai, F. Duan, Y. Zhang, and D. He. 2017. 'Fatigue Life Estimation of Medium-Carbon Steel with Different Surface Roughness', Applied Sciences, 7. Figure 1: Whole Life Rail Model (Burstow 2006).

Fatigue threshold

RCF

only RCF + wear Wear only

Where𝑆 is the applied stress [MPa], 𝑆𝑒 the endurance limit [MPa],𝐸 the Young’s modulus [MPa], 𝜈 the Poisson ratio [-], Ξ”πΎπ‘‘β„Ž the threshold of stress intensity factor [-], 𝐺 the shear

modulus [MPa],π‘Ž0 the initial crack size [mm],𝐢 the material constant, 𝛽1= 0.5 πœ‹ and 𝑛 empirical constants.

𝑁

𝑖

=

9 Ξ”πΎπ‘‘β„Ž 2𝐺 𝐸 π‘†βˆ’π‘†π‘’ 2πœ‹ 1βˆ’πœˆ π‘Ž0

𝑁

𝑝

=

π‘Ž0(1βˆ’π‘›2) 𝐢 𝑆𝑐𝛽1π‘›πœ‹π‘›2 𝑛 2βˆ’1 (3) (2)

The second part of the WLRM is when wear occurs and slip is involved. The preliminary approach to reconstruct this part is depicted in Figure 2. This flowchart shows the steps to determine the wear only threshold.

𝑁𝑓 = 𝑁𝑖+ 𝑁𝑝 (1)

Choose an initial contact condition with a certain wear number value

Determine the stress profiles within the material and the wear depth for one wheel passage

Determine whether surface of subsurface fatigue is dominant

Discretize stress profile and calculate wear depth as a function of the number of cycles

Determine at each element the number of cycles required for crack initiation using the S-N curve

If the π‘π‘π‘Ÿπ‘Žπ‘π‘˜ π‘–π‘›π‘–π‘‘π‘–π‘Žπ‘‘π‘–π‘œπ‘›= π‘π‘€π‘’π‘Žπ‘Ÿ π‘‘π‘’π‘π‘‘β„Ž

the wear only threshold is found

Figure 2: Flowchart to determine wear only threshold.

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