Chinese Journal of Lasers, Volume. 45, Issue 8, 802001(2018)
Effect of Directional Lorentz Force on Molten Pool Exhaust in Laser Cladding
Fig. 2. Powder morphology. (a) Powder microstructure; (b) internal hollow structure
Fig. 5. Lorentz force distributions in molten pool under different conditions. (a) Magnetic field strength of 0.6 T, current density of 5×106 A·m-2, upward Lorentz force; (b) magnetic field strength of 0.6 T, current density of 5×106 A·m-2, downward Lorentz force
Fig. 6. Flow field distributions in molten pool under different conditions. (a) Magnetic field strength of 0 T; (b) magnetic field strength of 0.6 T, current density of 5×106 A·m-2, Lorentz force is upward; (c) magnetic field strength of 0.6 T, current density of 5×106 A·m-2, Lorentz force is downward
Fig. 7. Trajectory map of bubbles with different diameters at different positions. (a) Front position; (b) middle position; (c) rear position; (d) statistical diagram of bubble park position
Fig. 8. Trajectory map of bubbles at different positions and under different Lorentz forces. (a) Point A position; (b) point B position; (c) point C position; (d) speed map along Y direction of bubble at point A
Fig. 9. Final park positions of bubble at different positions and under different Lorentz forces. (a) Point A position; (b) point B position; (c) point C position
Fig. 10. Distributions of pores in cladding layers under different conditions. (a) B=0 T; (b) B=0.3 T, upward Lorentz force; (c) B=0.6 T, upward Lorentz force; (d) B=0.3 T, downward Lorentz force; (e) B=0.6 T, downward Lorentz force
|
|
Get Citation
Copy Citation Text
Hu Yong, Wang Liang, Li Juehui, Zhang Qunli, Yao Jianhua, Volodymyr Kovalenko. Effect of Directional Lorentz Force on Molten Pool Exhaust in Laser Cladding[J]. Chinese Journal of Lasers, 2018, 45(8): 802001
Category: laser manufacturing
Received: Nov. 15, 2017
Accepted: --
Published Online: Aug. 11, 2018
The Author Email: