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Sensitivity analysis of melt pool - Finite Element prediction in laser cladding process of HSS material

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(1)

Sensitivity analysis of melt pool - Finite

Element prediction in laser cladding process

of HSS material

Ruben Jardin, Neda Hashemi, Hoang Son

Tran, Anne Mertens, Anne Marie Habraken

(2)

For High Speed Steel (M4 grade) wt%

Particle size [50 to 150 μm]

For thick deposit,

Direct Energy Deposition DED

process

or Laser cladding

 heterogeneity in melt pool

size in depth if no optimization

C Cr Mo V W Ni Si Fe

1.35 4.30 4.64 4.10 5.60 0.34 0.9 0.33

Research goal

(3)

Material High Speed Steel M4

• Fe-Cr-C-X alloys with X: carbide-forming element

(i.e. V, Mo or W)

• Hard carbides ⇒ High hardness and wear resistance

• Applications: high speed machining, cutting tools,

cylinders for hot rolling mills, molds...

(4)

Bulk Sample Laser beam speed (mm/s) 6.67

Laser power (W) 1100

Pre-heating (°C) 300

Mass flow (mg/s) 76

Number of tracks per layer 27

Total number of layers 36

Thin and bulk samples

40 x 40 x 27.5 mm (972 tracks) 2D FE model

(5)

Heat transfer by conduction

Heat transfer at boundary

• 𝑘 𝛻𝑇. 𝑛 = 𝑞𝑙𝑎𝑠𝑒𝑟 − ℎ 𝑇 − 𝑇0 − 𝜀𝜎 𝑇4 − 𝑇04

Latent heat of fusion

𝑐𝑝∗ = 𝐿𝑓 𝑇𝐷 − 𝑇 + 𝑐𝑝 int p T T T T k k k Q c x x y y z zt                  Heat Capacity Density

Power gen. per volume ( = 0 )

Convection Coef. Emissivity

Thermal equations

Conductivity

Laser Power

(6)

Active element Newly active element Inactive element Convection and radiation element

Element birth technique

(7)

2D mesh (convergence analysis)

Element size 0.75 mm

(8)

Last layer melt pool depth: 2.3 mm

Average layer height: 0.76 mm

Experimental results -> FE Validation

(9)

Parameters identification

• Fitting using the absorption factor of laser energy (β) and convection coef. (h);

(10)

Convection (h)

(W/m²K)

Emissivity (ε)

Absorption

factor (β)

Set

230

1

0.067

Simulation Parameters (boundary conditions)

(11)

Key heat transfers?

radiation

radiation + convection convection

(12)
(13)

Melt pool prediction/ layer

Bulk sample

T (K) Mid Height - 13.77 mm Depth 4.5 mm Depth 0.76 mm 3.1 re-melted layers 2.7 re-melted layers 2.0 re-melted layers

(14)

Sensitivity analysis

• Measured Thermo-physical parameters: k (±7%) ρ.cp (±3.6%) Lf

• A sensitivity analysis of melt pool size and thermal history to conductivity and heat capacity

• Which parameter is key?

(15)

Sensitivity to conductivity k

• Equilibrium at 150 s • 22 layers

• qlaser = qconv + qrad

(16)

Sensitivity to heat capacity ρc

p

• Long time to generate a layer • Strong convection

(17)

Melt pool depth prediction/ layer

Bulk sample

3.1 re-melted layers 2.7re-melted layers

2.0 re-melted layers Difference +7% k to -7% k = 0.46 mm (0.6 layer) 0 0.5 1 1.5 2 2.5 3 1 6 11 16 21 26 31 36 d e p th (mm) Layer number REF REF +3.6% ρcp REF -3.6% ρcp REF +7% k REF -7% k

(18)

Melt pool lenght prediction/ layer

Bulk sample

3.1 re-melted layers 2.7re-melted layers

Difference +7% k to -7% k = 1.41 mm Impact in amount of material added

2 3 4 5 6 7 8 1 6 11 16 21 26 31 36 le n gth (m m) layer number REF REF +3.6% ρcp REF -3.6% ρcp REF +7% k REF -7% k

(19)

Conclusion

 Thermo physical properties need accurate measurements  Critical to use temperature dependent properties and

analyse the impact of measurement error  2D model enough for bulk samples

(20)

Future on M4

 Use predicted thermal field

to optimize process parameters to keep constant melt pool size  more homogeneous microstructure

(21)

Questions?

Références

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