TY - JOUR
T1 - Crack formation law and mechanism in selective laser melting of 31gl stainless steels
AU - Pan, Lu
AU - Zhang, Chenglin
AU - Wang, Liang
AU - Liu, Qihui
AU - Wang, Gang
N1 - Publisher Copyright:
© 2019 Universitat zu Koln. All rights reserved.
PY - 2019
Y1 - 2019
N2 - Selective laser melting (SLM) is used to prepare 316L stainless steels. Further, the effects of laser power, scanning speed, and scanning spacing on the formation of cracks are studied in detail, the morphologies, chemical compositions, types of the precipitated phases, and grain sizes of the cracks are discussed, and the microstructures and formation mechanism of the cracks at different positions are presented. The results denote that the cracks mainly include micropore aggregation cracks, bubble aggregation cracks, and hot cracks. With the increase of linear energy density, the numbers of micropore aggregation cracks and bubble aggregation cracks are observed to initial increase and subsequent decrease; however, the number of hot cracks is observed to unidirectional increase. Under the optimal process parameters (a linear energy density of 222.2 J/m, a laser power of 200 W, and a laser scanning speed of 900 mm/s), the samples containing a small number of pores but no lacking cracks and no bubbles are obtained.
AB - Selective laser melting (SLM) is used to prepare 316L stainless steels. Further, the effects of laser power, scanning speed, and scanning spacing on the formation of cracks are studied in detail, the morphologies, chemical compositions, types of the precipitated phases, and grain sizes of the cracks are discussed, and the microstructures and formation mechanism of the cracks at different positions are presented. The results denote that the cracks mainly include micropore aggregation cracks, bubble aggregation cracks, and hot cracks. With the increase of linear energy density, the numbers of micropore aggregation cracks and bubble aggregation cracks are observed to initial increase and subsequent decrease; however, the number of hot cracks is observed to unidirectional increase. Under the optimal process parameters (a linear energy density of 222.2 J/m, a laser power of 200 W, and a laser scanning speed of 900 mm/s), the samples containing a small number of pores but no lacking cracks and no bubbles are obtained.
KW - Bubble
KW - Crack
KW - Defect analysis
KW - Laser technology
KW - Line energy density
KW - Pore
KW - Selective laser melting
UR - http://www.scopus.com/inward/record.url?scp=85065793795&partnerID=8YFLogxK
U2 - 10.3788/LOP56.101401
DO - 10.3788/LOP56.101401
M3 - Article
AN - SCOPUS:85065793795
SN - 1006-4125
VL - 56
JO - Laser and Optoelectronics Progress
JF - Laser and Optoelectronics Progress
IS - 9
ER -