Quenching Process for Spiral Bevel Gears Based on Thermo-Fluid-Solid Coupling Model

Introduction

Spiral bevel gears are critical components in mechanical transmission systems due to their high load-bearing capacity and smooth operation. However, their complex geometry and stringent performance requirements pose significant challenges during heat treatment, particularly in the quenching stage. Traditional trial-and-error methods for optimizing quenching processes are time-consuming and costly. This study proposes a novel numerical simulation framework that integrates thermo-fluid-solid coupling to eliminate the dependency on empirical heat transfer coefficients (HTCs). By coupling fluid dynamics with structural thermal-stress analysis, this approach enables accurate prediction of temperature distribution, phase transformation, and residual stress evolution in spiral bevel gears during quenching.


Methodology

1. Thermo-Fluid-Solid Coupling Framework

The quenching process involves interactions between the workpiece (spiral bevel gear), quenching medium, and thermal/mechanical fields. The governing equations for each domain are solved using a hybrid finite element method (FEM) and finite volume method (FVM):

Fluid Domain (FVM):

  • Mass Conservation:
    ∇⋅(αlρlul​)=0
  • Momentum Conservation:
    t∂(αlρlul​)​+∇⋅(αlρlulul​)=−αl​∇p+∇⋅τl​+αlρlg+Fdrag
  • Energy Conservation:
    t∂(αlρlhl​)​+∇⋅(αlρlulhl​)=∇⋅(αlkl​∇Tl​)+Sboil

Solid Domain (FEM):

  • Heat Conduction:
    ρscp​∂tTs​​=∇⋅(ks​∇Ts​)+qphase
  • Phase Transformation Kinetics:
    X=1−exp(−b(T)tn)
  • Elastoplastic Constitutive Model:
    σ=C🙁ϵϵthϵtp)

2. Boiling Heat Transfer Model

The Rensselaer Polytechnic Institute (RPI) wall boiling model accounts for three heat flux components during quenching:

  1. Single-phase convection:
    qconv​=hconv​(Tw​−Tl​)
  2. Evaporative latent heat:
    qevap​=6πdb3​fNwρghlg
  3. Transient conduction (“quenching”):
    qquench​=db​2klαlt/π​​(Tw​−Tl​)

3. Coupling Strategy

Data exchange between fluid and solid domains is achieved through:

  • Wall Functions:
    T+=qw​(Tw​−Tp​)ρCpuτ​​
  • Gauss Integration: Ensures flux continuity at fluid-solid interfaces.

Experimental Validation

1. Water Quenching of 45 Steel Cylinder

A cylindrical specimen (Φ25 mm × 100 mm) was quenched from 850°C to validate the model. Key measurements included:

ParameterMeasurement Technique
Cooling CurvesK-type Thermocouples
HardnessVickers Hardness Tester (HV1)
Residual StressX-ray Diffractometer
MicrostructureOptical Microscopy

2. Model Accuracy

The thermo-fluid-solid coupling model demonstrated excellent agreement with experiments:

MetricMax Relative Error
Cooling Rate9.2%
Surface Hardness3.6%
Residual Stress5.1%

Impact of Quenching Parameters on Spiral Bevel Gears

1. Flow Velocity Effects

Numerical simulations revealed that flow velocity (2 m/s optimal) significantly affects temperature uniformity and residual stress:

Flow Velocity (m/s)Final Cooling Position Offset (mm)Max Residual Stress (MPa)
1.02.79420
2.00.60380
3.01.15405

2. Medium Temperature Optimization

For 45 steel spiral bevel gears, quenching at 50°C balanced hardness and crack resistance:

Water Temp (°C)Surface Hardness (HV)Crack Probability (%)
3058018
505606
705403

Case Study: Spiral Bevel Gear Quenching

1. Geometry and Boundary Conditions

A Gleason-style spiral bevel gear (Module: 6, Teeth: 25) was modeled with adaptive meshing (Figure 1). Quenching oil (ISO VG 32) flow parameters were:

  • Inlet Velocity: 0.5–3.0 m/s
  • Turbulence Intensity: 5%
  • Initial Temp: 50°C

2. Simulation Results

  • Temperature Gradient: Tooth roots exhibited 15% faster cooling than dedendum surfaces due to flow stagnation.
  • Phase Distribution:
    M%=1−exp(−0.011(TMs​−T))
    Martensite content reached 92% at tooth tips vs. 78% at roots.
  • Residual Stress: Compressive stresses (-350 MPa) dominated at tooth surfaces, transitioning to tensile stresses (+280 MPa) in the core.

Discussion

  1. Advantages Over Traditional Methods:
    • Eliminates HTC measurement errors (±20–30% in industrial settings)
    • Captures localized boiling effects critical for spiral bevel gear distortion control
    • Reduces computational cost by 40% compared to fully resolved LES approaches
  2. Limitations:
    • Assumes isotropic material properties for martensite/ferrite phases
    • Requires calibration of RPI model constants for non-aqueous quenchants

Conclusion

The proposed thermo-fluid-solid coupling framework enables high-fidelity simulation of spiral bevel gear quenching processes. By resolving multiphase flow dynamics, phase transformations, and thermal stresses in a unified model, this approach provides:

  • Predictive capability for optimizing flow velocity (2 m/s) and medium temperature (50°C)
  • Quantitative assessment of residual stress and hardness distributions
  • Foundation for AI-driven quenching parameter optimization

Future work will integrate machine learning to automate parameter selection for complex spiral bevel gear geometries.


Key Equations Summary

Physical ProcessGoverning Equation
Martensite FormationM%=1−exp(−0.011(TMs​−T))
Heat Flux Partitioningqtotal​=qconv​+qevap​+qquench
Turbulent Kinetic Energyk=23​(UI)2(I=5%)
Phase Transformation RatedtdX​=nb(T)tn−1exp(−b(T)tn)

Material Properties of 45 Steel

PropertyAusteniteMartensiteFerrite
Density (kg/m³)805977857890
Thermal Conductivity (W/m·K)34.529.841.2
Specific Heat (J/kg·K)560620590
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