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School of Materials Science and Engineering Microstructural evolution and brazing mechanism of Ti 2 SnC-Ti6Al4V joint by using Cu pure foil Wenbo Yu, Shibo Li, Yann Aman, Zhipeng Guo, Shoumei Xiong School of materials science and engineering Tsinghua University Beijing China
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School of Materials Science and Engineering MAX phases M n+1 AX n [1] X: C and/or N A: A Group element M: Early transition metal Ceramic + Metal properties Edge-sharing [M 6 X] octahedra interleaved with A layers Good oxidation resistance Good damage tolerance [1] M.W. Barsoum et al.,, Progress in Solid State Chemistry, 28 (1-4), 201-281, 2000
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School of Materials Science and Engineering Pantograph: Good electrical conductivity Low friction coefficient Heating elements: Good oxidation resistance Motor: Low density Good resistance at high temperature Applications Al 2 O 3 TiC 0.67
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School of Materials Science and Engineering Background Crack healing 800 ℃ /1h Ti 2 SnC [2] Ti 2 SnC/Al 2 O 3 composite [3] [2] Li, S., et al.,. Journal of the European Ceramic Society, 2016. 36(1): p. 25-32. [3] Bei et al. J. Am. Ceram. Soc. 98 (2015)1604-1610
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School of Materials Science and Engineering sonication 10µm Widely biomedical application Such bone replacement 1200 ℃ /1h [4] Drawbacks: biotoxicity of vanadium Background [4] Gao et al.,. Journal of material research, 2002. 17(1): p. 25-32. [5] Zhao et al. Transaction nonferrous metal society. 2009 20(2)5p,414-417 Ti-6Al-4V 800 ℃ /1h [5 ] Possible: using Ti 2 SnC to replace Ti 3 SiC 2 The temperature can be strongly decreased
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School of Materials Science and Engineering Experimental procedure Ti, Sn, C powders with a molar ratio of 2:1:1 Sintering condition: 1250 ºC /30 MPa /1h in vacuum High-frequency induction heating device 750ºC /5MPa under Ar atmosphere
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School of Materials Science and Engineering layer I: migration of Cu atom into β-Ti layer II: Cu 4 Ti 3 Layer III : rich Cu and Ti Layer IV: CuTi 0.5 Sn 0.5 and Sn layer V: β-Cu(Sn) (bright area) and α-Cu(Sn) (grey area) Zhao et al. [5 ] 750ºC /5MPa/1h
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School of Materials Science and Engineering 750ºC /5MPa/20mins and 750ºC /5MPa/40mins EPMA results show Sn atoms began to accumulate adjacent to TC4 side Chemical compositions of layers I II and III did not change Sn began to accumulate between layer IV and V
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School of Materials Science and Engineering FIB procedure The side of Cu and Ti 2 SnC 1 In Fig(d), BSE images indicates two contrasts, Grain 1 was surrounded by white dots.
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School of Materials Science and Engineering TEM results Ti:Sn=1:0.73 Sn atoms diffuse out from Ti 2 SnC grains Cu atoms could diffuse into Ti 2 SnC grain boundaries and form Cu(Sn) solid solution.
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School of Materials Science and Engineering Shear test shear strength :85.7±10MPa. crack propagated in Ti 2 SnC Intergranular fracture mode.
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School of Materials Science and Engineering The side adjacent to Ti 2 SnC, Ti 2 SnC → xSn +Ti 2 Sn 1-x C (1) Sn +Cu → β-Cu (Sn) + α-Cu (Sn) (2) The side adjacent to TC4, the interdiffusion between Ti and Cu resulted into the following reaction. Cu + βTi → βTi (Cu) (layer I) (3) 3Ti +5Cu → Ti 3 Cu 4 layer (II) + Cu (Sn,Ti) (layer III) (4) With the increasing processing time, Sn atoms began to accumulate into Cu(Ti) layer and form CuTi 0.5 Sn 0.5 intermetallic. 1.5Sn + Cu (Ti) → Sn +CuTi 0.5 Sn 0.5 (layer IV) (5) Conclusions
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School of Materials Science and Engineering Thank you
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