Fatigue behavior under high frequency loading of materials produced by selective laser melting

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Abstract

Based on the enthalpy formulation of a three-dimensional transient nonlinear thermal conductivity problem for a multiphase system, mathematical modeling of the selective laser melting process of titanium and aluminum alloy powders was conducted to produce metallic components. The geometric parameters of a single track, as well as single-layer and multi-layer systems of overlapping tracks, were determined as functions of laser beam power and speed. This enabled the evaluation of the structure and types of defects arising during the layer-by-layer printing of samples. To investigate the influence of single and multiple defects on the fatigue strength of printed samples under high-frequency loading, a previously proposed multi-mode cyclic damage model was used. It was demonstrated that the internal heterogeneity of the microstructure of materials printed using selective laser melting can lead to earlier subsurface initiation of fatigue cracks, significantly reducing fatigue strength and durability. This effect is more pronounced in systems with multiple defects. The proposed models and computational algorithms enable the calculation of the fatigue strength and durability of samples for various defect systems in the microstructure, corresponding to the specified characteristics of the moving laser beam. They also make it possible to identify process parameters for selective laser melting that achieve the best fatigue strength performance under high-frequency loading.

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About the authors

I. S. Nikitin

Institute for Computer Aided Design of the RAS

Author for correspondence.
Email: i_nikitin@list.ru
Russian Federation, Moscow

N. G. Burago

Institute for Computer Aided Design of the RAS; Ishlinsky Institute for Problems in Mechanics RAS

Email: i_nikitin@list.ru
Russian Federation, Moscow; Moscow

A. D. Nikitin

Institute for Computer Aided Design of the RAS

Email: i_nikitin@list.ru
Russian Federation, Moscow

B. A. Stratula

Institute for Computer Aided Design of the RAS

Email: i_nikitin@list.ru
Russian Federation, Moscow

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Supplementary files

Supplementary Files
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1. JATS XML
2. Fig. 1. Graphical scheme of the problem of mobile heat flow from the laser beam 1 when it affects the powder layer 2 with the formation of a melt bath 6. The numeral 3 denotes the mobile phase boundary, 4 - substrate of material in solid phase, 5 - cooled laser trace in the form of material in solid phase.

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3. Fig. 2. Single SLP track in titanium alloy, q0 = 100 W, v = 800 mm/s, top view - a), cross-sectional view of the track and its fusion with the substrate - b), where w is the track width, d is the depth.

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4. Fig. 3. Results of calculations of track width w - a) and depth d - b) at different laser beam velocities v (mm/s) taking into account evaporation from the surface of the melt bath. Experimental data “1” from [1] are compared with the calculation results “2”.

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5. Fig. 4. Structure of the printed aluminum alloy observed in the electron microscope, (a) - top view, q0 = 370 W, v = 650 mm/s, electron microscope, (b) - cross-section of the near-surface layer, q0 = 370 W, v = 450 mm/s, optical microscope.

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6. Fig. 5. Overmelt zones (blue - 0 transitions, yellow - 3 transitions, orange - 4 transitions) for three-layer printing - (a), four-layer printing - (b).

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7. Fig. 6. Geometrical structure of overlapping tracks. Upper part - calculation, lower part - experiment, optical microscope.

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8. Figure 7. Defect structure results for titanium alloy, (a) - q0 = 50 W, v = 1000 mm/s, under-melting, (b) - q0 = 50 W, v = 500 mm/s, multiple remelts, no under-melts.

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9. Figure 8. Specimen with sharp notch without rounding - (a), meshes with characteristic cell size in the vicinity of the notch apex of 0.1 mm - (b), with 0.05 mm - (c).

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10. Fig. 9. Examples of calculation of quasi-cracks nucleation and development. Nucleation of a quasi-crack - (a), its development to a length of 1 mm - (b), its development to a length of 2 mm - (c).

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11. Figure 10. Number of cycles N before the nucleation of a crack from a sharp notch. Number of cycles as a function of mesh size h - a), normalized number of cycles - b). Curve 1 - without averaging procedure, curve 2 - with averaging.

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12. Figure 11. Defect systems in the specimen. Stress concentration on a linear defect system - a), stress concentration on a bilayer defect system - b).

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13. Fig. 12. Nucleation and development of a quasi-crack on a two-layer defect system. Nucleation, N =1.31E+09 - a), development, N =1.33E+09 - b).

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