Chinese Journal of Lasers, Volume. 47, Issue 11, 1102006(2020)

Local Shielding Gas Model for Laser Cladding of Titanium Alloy in Open Environment

Gong Yanqi, Fu Geyan*, Shi Tuo, Li Gang, Zhang Jinchao, and Yu Siqi
Author Affiliations
  • School of Mechanical and Electrical Engineering, Soochow University, Suzhou, Jiangsu 215021, China
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    Figures & Tables(16)
    Schematic of coaxial cladding nozzle
    Contour of oxygen distribution on substrate plane
    Schematic of the protection of high-temperature area around molten pool
    Cubic polynomial fitting curve
    Laser cladding system
    Residual normal probability distribution
    Correspondence between predicted value and actual value
    Results of single pass cladding confirmation tests
    • Table 1. Numerical simulation parameters and results

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      Table 1. Numerical simulation parameters and results

      No.Shielding gas flowrate Q /(L·min-1)Half effective protectionlength Leh /mm
      1185.70189775
      2217.76506575
      32410.03191600
      42712.06128200
      53013.52078375
      633.514.26290000
      73716.22803775
      840.516.86484750
      94418.30119650
      104719.27831025
      115020.21293800
    • Table 2. Significance analysis of fitting equation

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      Table 2. Significance analysis of fitting equation

      ItemDegree freedomSum of squaresMean squareF-valueP-value
      Model322.1054875.03516940.143941.7562×10-9
      Error70.558690.07981
      Total10225.66471
      R2=0.99752Adjusted R2= 0.99646
    • Table 3. Chemical composition of Ti-6Al-4V alloy substrate and powders

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      Table 3. Chemical composition of Ti-6Al-4V alloy substrate and powders

      MaterialMass fraction /%
      AlVFeCONHTi
      Substrate6.24.30.190.020.180.010.002Bal.
      Powder6.364.060.050.010.07850.00280.0012Bal.
    • Table 4. Impact factors level codes

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      Table 4. Impact factors level codes

      LevelFactor
      Plaser /Wv /(mm·s-1)f /mmvp /(r·min-1)Q /(L·min-1)
      -18504-40.714
      010506-3122
      112508-21.330
    • Table 5. BBD response surface experimental parameters and results

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      Table 5. BBD response surface experimental parameters and results

      No.Plaser /Wv /(mm·s-1)f /mmvp /(r·min-1)Q /(L·min-1)Lhtr /mm
      110504-412214.70684039
      212506-31.32212.18566775
      310508-31309.87459283
      410508-31.32210.71498371
      512504-312214.49674267
      610504-212212.60586319
      710506-312211.97557003
      810506-312212.60586319
      910506-312212.39576547
      1010508-412213.02605863
      1110508-311412.81596091
      1210506-312213.02605863
      1310506-413010.92508143
      1410506-30.71410.92508143
      158506-412213.23615635
      168506-313010.92508143
      1710506-312213.23615635
      1810506-40.72210.29478827
      1912506-30.72211.97557003
      2010504-31.32214.51250000
      218506-212210.71498371
      2210506-20.72210.92508143
      2312506-313015.75732899
      2410506-211414.28664495
      2510506-41.32211.97557003
      2612508-312212.39576547
      2710506-31.31412.18566775
      2810506-213010.92508143
      2910506-31.33011.76547231
      3012506-311414.07654723
      3110504-30.72211.13517915
      3210504-311413.65635179
      338506-311412.39576547
      3410506-21.32211.76547231
      3510506-312211.55537459
      3610504-313013.65635179
      378508-31229.87459283
      388506-31.32210.29478827
      3910506-411413.65635179
      4010508-212210.50488599
      4112506-412214.07654723
      4212506-212212.81596091
      438504-312213.02605863
      4410506-30.73011.76547231
      458506-30.7229.24429967
      4610508-30.72210.08469055
    • Table 6. Significance analysis of response value model coefficients and lack of fit

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      Table 6. Significance analysis of response value model coefficients and lack of fit

      SourceP-valueLack of fitP-valueResult
      Linear<0.00010.0973Suggested
      2FI0.78050.0755
      Quadratic0.00630.1711Suggested
      Cubic0.11480.3324Aliased
    • Table 7. Anova of quadratic regression model for the length of high temperature area behind the spot center

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      Table 7. Anova of quadratic regression model for the length of high temperature area behind the spot center

      SourceSum of squaresDegree of freedomMean squareF valueP-value>FRemark
      Model78.3998.7113.46<0.0001Significant
      Plaser20.40120.4031.53<0.0001
      v21.40121.4033.07<0.0001
      f3.3813.385.220.0283
      vp5.1215.127.910.0079
      Q4.4114.416.820.0131
      PlaserQ2.4812.483.840.0579
      vvp1.8911.892.920.0964
      vQ2.1612.163.340.0758
      vp217.14117.1426.48<0.0001
      Residual23.30360.65
      Lack of fit21.29310.691.720.2870Not significant
      Pure error2.0050.40
      Cor total101.6845
      R2=0.7709Adjusted R2=0.7136Predicted R2=0.6002Adeq Precisior=14.030
    • Table 8. Process parameters and results of confirmation tests

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      Table 8. Process parameters and results of confirmation tests

      No.Plaser /Wv /mmf /mmvp /(r·min-1)Qmin /(L·min-1)Qadj /(L·min-1)Lhtr,P/mmLhtr,R /mmLeh /mmError /%
      112504-4143.71854418.13068316.77487518.184450617.48
      212504-31.341.13924217.39250216.28906517.553587866.34
      312004-31.139.04824016.72169315.52031716.926998007.18
      412505-4137.11763816.06861015.31875016.288115664.67
      512505-31.334.04453515.00018415.01640815.270507000.11
      611504-40.832.11793314.24771514.06250014.528419941.30
      711005-21.129.91403013.24189812.20625013.278354007.82
      812507-21.227.80752812.23216411.95313012.329528622.28
      910007-3125.94772611.23538410.43086511.269018517.16
      109007-21.223.8533249.9637659.60937510.080258293.56
      118508-21.321.7335228.4929148.6375008.746682581.70
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    Gong Yanqi, Fu Geyan, Shi Tuo, Li Gang, Zhang Jinchao, Yu Siqi. Local Shielding Gas Model for Laser Cladding of Titanium Alloy in Open Environment[J]. Chinese Journal of Lasers, 2020, 47(11): 1102006

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    Paper Information

    Category: laser manufacturing

    Received: Feb. 24, 2020

    Accepted: --

    Published Online: Nov. 9, 2020

    The Author Email: Fu Geyan (fugeyan@suda.edu.cn)

    DOI:10.3788/CJL202047.1102006

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