Real-time in-focus CO2 and fiber laser beam optimization with a twin hexapod operated beam expander and fully automated beam analysis with simultaneous raw and focused beam measurement

Author(s):  
Murad Jamalieh ◽  
Markus Bohrer
2021 ◽  
pp. 103786
Author(s):  
Dongdong Han ◽  
Yijie Wang ◽  
Zhanqiang Hui ◽  
Zhixing Zhang ◽  
Kaili Ren ◽  
...  

2008 ◽  
Author(s):  
Steffen Mueller ◽  
Craig Bratt ◽  
Peter Mueller ◽  
Jonathan Cuddy ◽  
Kartik Shankar

2013 ◽  
Author(s):  
Haotong Ma ◽  
Haojun Hu ◽  
Wenke Xie ◽  
Guangwen Jiang ◽  
Xiaojun Xu

2021 ◽  
Vol 70 (20) ◽  
pp. 204203-204203
Author(s):  
Zhang Yu-Qiu ◽  
◽  
Huang Liang-Jin ◽  
Chang Qi ◽  
An Yi ◽  
...  

2015 ◽  
Vol 9 (4) ◽  
pp. 265-269 ◽  
Author(s):  
Wojciech Cieszyński ◽  
Michał Zięba ◽  
Jacek Reiner

Abstract Application of laser welding technology requires that the laser beam is guided through the whole length of the joint with sufficiently high accuracy. This paper describes result of research on development of optomechatronic system that allows for the precise positioning of the laser head’s TCP point on the edge of welded elements during laser processing. The developed system allows for compensation of workpiece’s fixture inaccuracies, precast distortions and workpiece deformations occurring during the process.


Author(s):  
Mohit Singh ◽  
Sanjay Mishra ◽  
Vinod Yadava ◽  
J. Ramkumar

Laser beam percussion drilling (LBPD) can create high density holes in aerospace materials with the repeated application of laser pulses at a single spot. In this study, one-parameter-at-a-time approach has been used to investigate the individual effect of peak power, pulse width and pulse frequency on geometrical accuracy and metallurgical distortion during LBPD of 0.85[Formula: see text]mm thick Ti–6Al–4V sheet using 200[Formula: see text]W Yb:YAG fiber laser. It has been found that the output parameters behave differently at the higher and lower values of a particular input process. The increase of pulse width from 1 to 1.50[Formula: see text]ms increases hole taper by 20% whereas the same corresponding change from 1.50 to 2.00[Formula: see text]ms reduces the taper by 20%. The increase of pulse frequency from 10 to 50[Formula: see text]Hz reduces hole circularity by 40% but the same proportionate change from 50 to 90[Formula: see text]Hz reduces circularity by 79%. Increase of peak power from 1.70 to 2.0[Formula: see text]kW increases hole taper by 8% but the corresponding increase from 2 to 2.30[Formula: see text]kW is 143%.


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