Chinese Journal of Lasers, Volume. 51, Issue 16, 1602409(2024)

Monte Carlo Simulation and Experimental Investigation of Back Strike Protection in Laser Drilling

Qingyang Zeng1,2,3, Bin Wang1,2, and Wenwu Zhang1,2、*
Author Affiliations
  • 1Ningbo Institute of Materials Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, Zhejiang , China
  • 2Zhejiang Key Laboratory of Aero Engine Extreme Manufacturing Technology, Ningbo 315201, Zhejiang , China
  • 3University of Chinese Academy of Sciences, Beijing 100049, China
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    Figures & Tables(16)
    Schematics of the computational and random value domains (figures have been scaled to be easier to read). (a) p<t; (b) p≥t
    Variation of Monte Carlo simulation results with amount of data. (a1)(a2) Diameter of protective material particles p=0.05 mm; (b1)(b2) p=0.3 mm; (c1)(c2) p=0.7 mm
    Violin diagram of Monte Carlo simulation results for blocking rate
    Schematics of the laser processing system and the back strike protection. (a) Laser processing system; (b) without protective material; (c) with protective material
    Schematics of test piece and measuring result of typical back strike pit (400×, standard order No.5). (a) Schematic of test piece;
    Main effects plots for depth of back strike pit
    Schematic of the breakthrough timing experiment
    Processing of calculating breakthrough time from the video frames. (a) SiC; (b) graphite; (c) ZrO2; (d) Al alloy front wall
    Breakthrough time comparison of different materials
    • Table 1. Algorithm process of Monte Carlo simulation

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      Table 1. Algorithm process of Monte Carlo simulation

      Monte Carlo simulation: overlap area between laser processing area and protective particles

      input: Diameter of protective material particles P =[p1p2p3, ···, pi, ···, pn]; Diameter of laser drilling t; Groups of particle diameter n; Maximum of Monte Carlo simulations for each set of particle diameters Nmax

      output: overlap area data matrix O

      1: Initialize the overlap area data matrix O in n×Nmax

      2: fori=1, 2, ···, n do

      3: ifPi)<t do

      4: The calculation area, particle arrangement, and drop range are constructed according to Fig. 1(a);

      5: elsedo

      6: The calculation area, particle arrangement, and drop range are constructed according to Fig. 1(b);

      7: end if

      8: Generate Nmax×2 randomized drop matrices within the drop range [XY]=[x1y1x2y2···xkyk···xNmaxyNmax];

      9: Initialize loop variable k=1;

      10: whilekNmax do

      11: Calculate the overlap area oik between the laser processing region centered at [XY](k ) and the shape of particles;

      12: Oik)=oik

      13: k=k+1;

      14: end while

      15: end for

      16: return O

    • Table 2. Parameters of the laser source and optical component

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      Table 2. Parameters of the laser source and optical component

      ParameterValue
      Wavelength /nm532.0
      Average power /W≤32.9
      Pulse repetition rate /kHz10.0‒50.0
      Pulse width /ns≥23.2
      Focus length /mm163.0
      Spot size /μm30.65
    • Table 3. Physical and chemical properties of filling materials

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      Table 3. Physical and chemical properties of filling materials

      MaterialPhysical formMolar mass /(g/mol)Density /(g/m³)Melting point /℃Boiling point /℃
      Graphite (C)Black irregular crystals12.0112.204489 (10.4 MPa)3825 (sublimation point)
      Zirconium oxide (ZrO2White spherical powder123.2235.6827104300
      Silicon carbide (SiC)Green-black irregular crystals40.0973.162830
    • Table 4. Chemical composition of 6061 aluminum alloy and GH3536 nickel-based superalloy

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      Table 4. Chemical composition of 6061 aluminum alloy and GH3536 nickel-based superalloy

      MaterialMass fraction /%
      SiFeCuMgCoCrMoOther elementsBal.
      60610.4‒0.80.70.15‒0.400.8‒1.20.04‒0.35

      Ti: 0.15; Mn: 0.15;

      Zn: 0.25

      Al
      GH35360.3318.760.021.3220.946.64

      Al: 0.40; W: 0.86;

      Mn: 0.61; C: 0.08

      Ni
    • Table 5. Factor level setting table

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      Table 5. Factor level setting table

      LevelA (material, text factor)B (binder, text factor)C (pulse repetition rate /kHz)D (processing time /s)
      -1ZrO2 (spherical)Not added102
      0306
      1SiC (irregular)Added5010
    • Table 6. Screening DOE design and experimental results

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      Table 6. Screening DOE design and experimental results

      Standard orderA (material, text factor)B (binder, text factor)C (pulse repetition rate /kHz)D (processing time /s)Response (depth of back strike pit /μm)
      1SiCAdded5010207.46
      2ZrO2Not added1020
      3ZrO2Not added502298.61
      4SiCAdded10100
      5ZrO2Added3010427.93
      6SiCNot added3020
      7ZrO2Not added506300.10
      8SiCAdded1060
      9ZrO2Not added1010331.38
      10SiCAdded5020
      11ZrO2Added1020
      12SiCNot added5010478.98
      13SiCNot added306270.37
      14ZrO2Added306421.99
    • Table 7. ANOVA and significance test for the model of depth of back strike pit

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      Table 7. ANOVA and significance test for the model of depth of back strike pit

      SourceDegrees of freedomAdjusted mean squaresF-valueP-valueSignificance level
      Model76155612.350.0035**
      Linear48924517.910.0017**
      A (material)110134720.340.0041**
      B (binder)1172993.470.1117
      C (pulse repetition rate)110443720.960.0038**
      D (processing time)118558437.240.0009**
      Square16507013.060.0112*
      C×C16507013.060.0112*
      2-way interactions2169213.400.1032
      A×D1126712.540.1619
      B×D1312216.270.0463*
      Error64983
      Total13
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    Qingyang Zeng, Bin Wang, Wenwu Zhang. Monte Carlo Simulation and Experimental Investigation of Back Strike Protection in Laser Drilling[J]. Chinese Journal of Lasers, 2024, 51(16): 1602409

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    Paper Information

    Category: Laser Micro-Nano Manufacturing

    Received: Oct. 23, 2023

    Accepted: Dec. 5, 2023

    Published Online: Jul. 29, 2024

    The Author Email: Zhang Wenwu (zhangwenwu@nimte.ac.cn)

    DOI:10.3788/CJL231321

    CSTR:32183.14.CJL231321

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