LASER SHOCK PROCESSING OF Ti-6Al-4V AND ANALYSIS OF ITS MICROSTRUCTURE RESPONSE
LUO Xinmin1), ZHAO Guangzhi1), ZHANG Yongkang2), CHEN Kangmin1, 3), LUO Kaiyu2), REN Xudong2)
1) School of Material Science and Engineering, Jiangsu University, Zhenjiang 212013
2) School of Mechanical Engineering, Jiangsu University, Zhenjiang 212013
3) Analysis and Test Center, Jiangsu University, Zhenjiang 212013
Cite this article:
LUO Xinmin ZHAO Guangzhi ZHANG Yongkang CHEN Kangmin LUO Kaiyu REN Xudong. LASER SHOCK PROCESSING OF Ti-6Al-4V AND ANALYSIS OF ITS MICROSTRUCTURE RESPONSE. Acta Metall Sin, 2012, 48(9): 1116-1122.
Abstract Laser shock processing (LSP) is an effective and promising technology for improving surface mechanical properties of metals. The study of the strain behavior of individual phase of advanced engineering materials with polycrystalline and dual-phase microstructures subjected to laser shock processing is an important emerging frontier, which facilitates understanding of the relative roles of intrinsic and extrinsic attributes of microstructure upon strengthening, compared with the strengthening process of metals at the macroscopic scale of deformation. The influence of LSP on the surface layer properties and microstructures of a Ti-6Al-4V alloy has been investigated focusing on the microstructure response of the surface layer of the alloy by means of high efficient Nd3+∶YAG ceramic pulse laser with 12.5 J per pulse at 1064 nm and 10 Hz repetition rate. The microstructures response of the alloy are analyzed and characterized with by FE-SEM, TEM and the inverse fast fourier transform (IFFT) algorithm, respectively. The experimental results show that the surface hardness of the laser shocked Ti-6Al-4V alloy can increase 80%, and the compressive residual stress can be over\linebreak 500 MPa. Obvious preference effect between α and β phase is discovered upon strengthening of the alloy under the conditions of the ultra high energy and ultra-high strain rate of laser shock. With the lower shock energy, the deformation strengthening of β phase takes precedence over the other; as the shock energy increasing, both α and β are strengthened simultaneously, whereas, the previously strengthened β phase shows saturated strengthening effect. The results also reveal that dislocation multiplication is the main strengthen mechanism in the laser shocked region, including oriented dislocation projection and dislocation dipoles in the α phase with hcp crystal lattice, but diversified configurations, such as edge-dislocation, extended dislocations and dislocation dipoles presenting in the β phase with bcc crystal lattice. The semi-coherent interface with misfit dislocations between α and β phase boundary is discovered, which plays a synergetic role upon deformation strengthening. Additionally, the strain screening manifestation within the laser shocked region is also discussed, which is regarded as a kind of self-organization phenomenon of deformation defects, and can be attributed to the synthetic effect of the confinement conditions upon laser shocking, the accumulative strengthening mode of single-spot laser shocking process and the differences of strength and crystalline structure between the lamellar α and β phases.
[16] Luo X M, Zhang Y K, Chen K M, Ren X D. In: Slabe J M ed., Proc 8th Int Conf zIndustral Tools and Material Processing Technologies{, Ljubljana: Ljubljana University, 2011: 223
[17] Luo X M, Zhao G Z, Yuan C Z, Zhang Y K, Chen K M. In: BobWed., Proc ICMTMA 2011. Los Alamitos: IEEE Computer Society, 2011: 556
[18] Rozmus G M. Acta Phys Polonica, 2010; 117A: 808
[19] Christoph L, Manfred P. Titanium and Titanium Alloys: Fundamentals and Applications. Weinheim: WILEY– VCH Verlag GmbH & Co. KGaA, 2003: 1
[20] Tao C H, Liu Q Q, Cao C X, Zhang W F. Failure and Prevention of Aeronautical Titanium Alloy. Beijing: National Defense Industry Press, 2002: 11
