• Laser & Optoelectronics Progress
  • Vol. 55, Issue 11, 111601 (2018)
Wendan Tan1、**, Ming Pang1、*, Guoye Jiang1, Wei Fu1, Xiaohan Zhang1, Dingyun Hu2, Jing Cui1, and Guangfeng Yang1
Author Affiliations
  • 1 Airport College, Civil Aviation University of China, Tianjin 300300, China
  • 2 China North Engine Research Institute, Tianjin 300400, China
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    DOI: 10.3788/LOP55.111601 Cite this Article Set citation alerts
    Wendan Tan, Ming Pang, Guoye Jiang, Wei Fu, Xiaohan Zhang, Dingyun Hu, Jing Cui, Guangfeng Yang. Numerical Simulation of Temperature Field in Laser Phase-Transformation Hardening of Highly-Enhanced Diesel Engine Valve Seats[J]. Laser & Optoelectronics Progress, 2018, 55(11): 111601 Copy Citation Text show less
    Three-dimensional finite element mesh model of valve seat
    Fig. 1. Three-dimensional finite element mesh model of valve seat
    Temperature field of laser phase-transformation hardening of valve seat versus time. (a) t=0.09 s; (b) t=5.4 s; (c) t=10.8 s
    Fig. 2. Temperature field of laser phase-transformation hardening of valve seat versus time. (a) t=0.09 s; (b) t=5.4 s; (c) t=10.8 s
    Sectional temperature distribution of valve seat at t=10.8 s. (a) Temperature field distribution; (b) temperature contour plot
    Fig. 3. Sectional temperature distribution of valve seat at t=10.8 s. (a) Temperature field distribution; (b) temperature contour plot
    Thermal cycle curves for different nodes in phase-transformation hardening area of valve seat at t=5.13 s
    Fig. 4. Thermal cycle curves for different nodes in phase-transformation hardening area of valve seat at t=5.13 s
    Thermal cycle curves at peak temperature points corresponding to different time along scanning direction
    Fig. 5. Thermal cycle curves at peak temperature points corresponding to different time along scanning direction
    Temperature field distributions of valve seat for different laser powers. (a) P=1000 W; (b) P=900 W; (c) P=800 W; (d) P=700 W
    Fig. 6. Temperature field distributions of valve seat for different laser powers. (a) P=1000 W; (b) P=900 W; (c) P=800 W; (d) P=700 W
    Peak temperature of valve seat and depth & width of hardened layer versus laser power. (a) Peak temperature of valve seat; (b) depth & width of hardened layer
    Fig. 7. Peak temperature of valve seat and depth & width of hardened layer versus laser power. (a) Peak temperature of valve seat; (b) depth & width of hardened layer
    Temperature field distribution of valve seat versus laser scanning speed. (a) V=5 mm·s-1; (b) V=8 mm·s-1; (c) V=10 mm·s-1; (d) V=15 mm·s-1
    Fig. 8. Temperature field distribution of valve seat versus laser scanning speed. (a) V=5 mm·s-1; (b) V=8 mm·s-1; (c) V=10 mm·s-1; (d) V=15 mm·s-1
    Peak temperature of valve seat and depth & width of hardened layer versus scanning speed. (a) Peak temperature of valve seat; (b) depth & width of hardened layer
    Fig. 9. Peak temperature of valve seat and depth & width of hardened layer versus scanning speed. (a) Peak temperature of valve seat; (b) depth & width of hardened layer
    Temperature distribution in phase-transformation hardening area of valve seat versus laser spot radius
    Fig. 10. Temperature distribution in phase-transformation hardening area of valve seat versus laser spot radius
    Schematic of path nodes in inclined plane
    Fig. 11. Schematic of path nodes in inclined plane
    Temperature field distributions for different laser spot radii. (a) R=1.0 mm; (b) R=1.2 mm; (c) R=1.5 mm; (d) R=1.6 mm
    Fig. 12. Temperature field distributions for different laser spot radii. (a) R=1.0 mm; (b) R=1.2 mm; (c) R=1.5 mm; (d) R=1.6 mm
    Peak temperature of valve seat and depth & width of hardened layer for different laser spot radii. (a) Peak temperature of valve seat; (b) depth & width of hardened layer
    Fig. 13. Peak temperature of valve seat and depth & width of hardened layer for different laser spot radii. (a) Peak temperature of valve seat; (b) depth & width of hardened layer
    Morphology of hardened layer
    Fig. 14. Morphology of hardened layer
    Depth and width of hardened layer obtained by numerical simulation and experiment
    Fig. 15. Depth and width of hardened layer obtained by numerical simulation and experiment
    Temperature T /℃Thermal diffusioncoefficient /(mm2·s-1)Heat conductivity coefficientλ /(W·m-1·K-1)Specific heatcapacity c /(J·g-1·K-1)
    2512.85942.3700.465
    20011.02043.3390.555
    4008.97641.0250.645
    5007.97539.3320.696
    6006.81838.0220.787
    Table 1. Thermophysical parameters of RuT300
    ElementCSiMnPSFe
    Content3.5-3.92.2-2.80.4-0.8<0.06<0.04Bal.
    Table 2. Chemical compositions of RuT300 (mass fraction, %)
    Wendan Tan, Ming Pang, Guoye Jiang, Wei Fu, Xiaohan Zhang, Dingyun Hu, Jing Cui, Guangfeng Yang. Numerical Simulation of Temperature Field in Laser Phase-Transformation Hardening of Highly-Enhanced Diesel Engine Valve Seats[J]. Laser & Optoelectronics Progress, 2018, 55(11): 111601
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