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SIMULATIONS OF THERMO-MECHANICAL
      CHARACTERISTICS IN ELECTRON BEAM
       ADDITIVE MANUFACTURING (EBAM)

                           Ninggang (George) Shen
                               Dr. Kevin Chou

                                 11/14/2012




The University of Alabama-Mechanical Engineering    1
Outline of the contents

1. Introduction

2. Thermo-mechanical modeling

3. FE model application

4. Thermo-mechanical analysis

5. Conclusions

6. Future work




The University of Alabama-Mechanical Engineering   2
1. Introduction and research objectives


What’s Electron Beam Additive Manufacturing (EBAM)?
  • Metallic powders melt by electron beam
  • Rapid self-cool to solidify
  • Produced in layer-building fashion

 Why EBAM?
  • Be able to build full-density functional metallic products
  • Eco-friendly
  • High building rate (Ti-6Al-4V: 25-50 cm3/hour [1])




The University of Alabama-Mechanical Engineering                 3
1. Introduction and research objectives

Powder materials
 • Study of porosity effects on heat transfer
   Metallic powders are preheated to slightly sintered before each deposition;
   Porosities in powder bed affect thermal response very much




    Fig. 1 SEM picture of Ti-6Al-4V powder          Fig 2. SEM picture of sintered Ti-6Al-4V powder

The University of Alabama-Mechanical Engineering                                                      4
1. Introduction and research objectives

Potential part quality problem in EBAM:
 • Delamination
  The induced residual stresses are greater than the bonding ability between layers




                               Fig. 3 Delamination [2]

The University of Alabama-Mechanical Engineering                                      5
1. Introduction and research objectives

A 3D Finite Element (FE) thermo-mechanical model
 was developed to:
 • Investigate the thermo-mechanical response in EBAM
 • Behavior of thermal and residual stress
 • Deformation analysis




The University of Alabama-Mechanical Engineering        6
2. Thermo-mechanical modeling

  Assumptions:
    • Conical volumetric body heat flux
    • Gaussian intensity distribution in deposition plane
    • Linear decay along penetration




Fig. 4 Actual keyhole example and idealization [3]      Fig. 5 Horizontal intensity distribution @ z = 0


  The University of Alabama-Mechanical Engineering                                                         7
2. Thermo-mechanical modeling




Fig. 4 Thermal & mechanical bulk material materials [4,5]   Fig. 5 Thermal conductivity of both bulk and powder




   The University of Alabama-Mechanical Engineering                                                        8
2. Thermo-mechanical modeling


       Tab. 1 Truth table of material determination
                             DTemp > 0           DTemp < 0


    Temp < Tmelting             0                   0


    Temp > Tmelting             0                   1

  †0 – powder, 1 – solid

• Latent heat of fusion is considered as well




                           Fig. 6 Flow chart of the user subroutine
                                  coupled UMATH and DFLUX

The University of Alabama-Mechanical Engineering                      9
3. FE model application

                                                   Tab. 2 Parameters in the melting simulation
                                              Parameters                                  Values
                                              Solidus temperature, TS ( C)                 1605
                                              Liquidus temperature, TL ( C)                1665
                                              Latent heat of fusion, Lf (kJ/Kg)                440
                                              Electron beam diameter, Φ (mm)                   0.4
                                              Absorption efficiency, η                         0.9
                                              Scan speed, v (m/sec)                            0.4
                                              Acceleration voltage, U (kV)                      60
                                              Beam current, Ib (mA)                              2
                                              Powder layer thickness, t-layer (mm)             0.1
                                              Porosity, φ                                   30%
                                              Beam penetration depth, dP (mm)                  0.1
        Fig. 7 New FE model configuration
                                              Preheat temperature, Tpreheat ( C)               750




The University of Alabama-Mechanical Engineering                                          10
3. FE model application




Fig. 8 Schematic of the cross-raster scan pattern
applied in the multi-layer EBAM thermal
analysis.




     The University of Alabama-Mechanical Engineering   11
4. Thermo-mechanical analysis




                                                          Fig. 10 the simulated residual stress profile comparison




Fig. 9 the simulated temperature contour comparison


                                                      Fig. 11 the simulated residual stress distribution comparison
 The University of Alabama-Mechanical Engineering                                                          12
4. Thermo-mechanical analysis




Fig. 12 Simulated temperature fields and molten pool   Fig. 13 Simulated temperature fields and molten pool
geometry.                                              geometry for raster scan: a) the temperature fields of
                                                       layer-1; b) the cross sectional view of the field in a).

    The University of Alabama-Mechanical Engineering                                                     13
4. Thermo-mechanical analysis




Fig. 14 Simulated temperature history and thermal
stress histories close the beam center starting point.   Fig. 15 Simulated thermal stress fields of single straight scan
                                                         just before cooling: a) Longitudinal stress; b) Transverse stress.

    The University of Alabama-Mechanical Engineering                                                              14
4. Thermo-mechanical analysis




                Fig. 16 Simulated residual stress fields of single straight
                    scan: a) Longitudinal stress; b) Transverse stress.




The University of Alabama-Mechanical Engineering                              15
4. Thermo-mechanical analysis




Fig. 17 Simulated thermal stress and its cross sectional view.


                                                                 Fig. 18 Simulated thermal stress fields and their cross
                                                                 sectional views at the end of the 10 sec break between
                                                                 two sequential layers: a) Longitudinal stress; b)
                                                                 Transverse stress.


    The University of Alabama-Mechanical Engineering
4. Thermo-mechanical analysis




Fig. 19 Simulated residual stress fields and their cross
sectional views: a) Longitudinal stress; b) Transverse
stress.


                                                           Fig. 20 Simulated deformations (mm) for: a) Single straight
                                                           scan; b) Multi-layer crossed raster scan.



 The University of Alabama-Mechanical Engineering
5. Conclusions

• The raster scan pattern affects the temperatures and molten pool due to the
 residual heat from previous adjacent scan

• Thermal stress histories on top (for both longitudinal and transverse)
   Compressive – just before beam coming; Tensile - solidified

• Vertical thermal stress distribution (for both longitudinal and transverse)
   Tensile in solidified and the compressive just beneath the tensile

• Vertical residual stress distribution (for both longitudinal and transverse)
   Max. tensile in solidified and it decreases to the compressive for a certain penetration.

• The largest deformation follows the track of beam center




The University of Alabama-Mechanical Engineering                                               18
6. Future work




                              Fig. 21 Hatch melting




The University of Alabama-Mechanical Engineering      19
Acknowledgement

Sponsor: NASA, No. NNX11AM11A
Collaborator: Marshall Space Flight Center (Huntsville, AL),
              Advanced Manufacturing Team.




 The University of Alabama-Mechanical Engineering         20
Q&A



 Thank you for your attention!

                    Any Question?




The University of Alabama-Mechanical Engineering   21
Reference
[1] Available from: http://www.arcam.com/.
[2] Zaeh, M. F., and Lutzmann, S., 2010, "Modelling and simulation of electron beam melting," Production
    Engeering. Research and Development, 4, pp. 15-23.
[3] Lampa, C., Kaplan, A. F. H., Powell, J., and Magnusson, C., 1997, "An analytical thermodynamic model of laser
    welding," Journal of Physics D: Applied Physics, 30(9), p. 1293.
[4] Yang, J., Sun, S., Brandt, M., and Yan, W., 2010, "Experimental investigation and 3D finite element prediction
    of the heat affected zone during laser assisted machining of Ti6Al4V alloy," Journal of Materials Processing
    Technology, 210(15), pp. 2215-2222.
[5] Liu, C., Wu, B., and Zhang, J., 2010, "Numerical Investigation of Residual Stress in Thick Titanium Alloy Plate
    Joined with Electron Beam Welding," Metallurgical and Materials Transactions B, 41(5), pp. 1129-1138.




  The University of Alabama-Mechanical Engineering                                                             22

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Simulations of Thermo-Mechanical Characteristics in Electron Beam Additive Manufacturing

  • 1. SIMULATIONS OF THERMO-MECHANICAL CHARACTERISTICS IN ELECTRON BEAM ADDITIVE MANUFACTURING (EBAM) Ninggang (George) Shen Dr. Kevin Chou 11/14/2012 The University of Alabama-Mechanical Engineering 1
  • 2. Outline of the contents 1. Introduction 2. Thermo-mechanical modeling 3. FE model application 4. Thermo-mechanical analysis 5. Conclusions 6. Future work The University of Alabama-Mechanical Engineering 2
  • 3. 1. Introduction and research objectives What’s Electron Beam Additive Manufacturing (EBAM)? • Metallic powders melt by electron beam • Rapid self-cool to solidify • Produced in layer-building fashion Why EBAM? • Be able to build full-density functional metallic products • Eco-friendly • High building rate (Ti-6Al-4V: 25-50 cm3/hour [1]) The University of Alabama-Mechanical Engineering 3
  • 4. 1. Introduction and research objectives Powder materials • Study of porosity effects on heat transfer Metallic powders are preheated to slightly sintered before each deposition; Porosities in powder bed affect thermal response very much Fig. 1 SEM picture of Ti-6Al-4V powder Fig 2. SEM picture of sintered Ti-6Al-4V powder The University of Alabama-Mechanical Engineering 4
  • 5. 1. Introduction and research objectives Potential part quality problem in EBAM: • Delamination The induced residual stresses are greater than the bonding ability between layers Fig. 3 Delamination [2] The University of Alabama-Mechanical Engineering 5
  • 6. 1. Introduction and research objectives A 3D Finite Element (FE) thermo-mechanical model was developed to: • Investigate the thermo-mechanical response in EBAM • Behavior of thermal and residual stress • Deformation analysis The University of Alabama-Mechanical Engineering 6
  • 7. 2. Thermo-mechanical modeling Assumptions: • Conical volumetric body heat flux • Gaussian intensity distribution in deposition plane • Linear decay along penetration Fig. 4 Actual keyhole example and idealization [3] Fig. 5 Horizontal intensity distribution @ z = 0 The University of Alabama-Mechanical Engineering 7
  • 8. 2. Thermo-mechanical modeling Fig. 4 Thermal & mechanical bulk material materials [4,5] Fig. 5 Thermal conductivity of both bulk and powder The University of Alabama-Mechanical Engineering 8
  • 9. 2. Thermo-mechanical modeling Tab. 1 Truth table of material determination DTemp > 0 DTemp < 0 Temp < Tmelting 0 0 Temp > Tmelting 0 1 †0 – powder, 1 – solid • Latent heat of fusion is considered as well Fig. 6 Flow chart of the user subroutine coupled UMATH and DFLUX The University of Alabama-Mechanical Engineering 9
  • 10. 3. FE model application Tab. 2 Parameters in the melting simulation Parameters Values Solidus temperature, TS ( C) 1605 Liquidus temperature, TL ( C) 1665 Latent heat of fusion, Lf (kJ/Kg) 440 Electron beam diameter, Φ (mm) 0.4 Absorption efficiency, η 0.9 Scan speed, v (m/sec) 0.4 Acceleration voltage, U (kV) 60 Beam current, Ib (mA) 2 Powder layer thickness, t-layer (mm) 0.1 Porosity, φ 30% Beam penetration depth, dP (mm) 0.1 Fig. 7 New FE model configuration Preheat temperature, Tpreheat ( C) 750 The University of Alabama-Mechanical Engineering 10
  • 11. 3. FE model application Fig. 8 Schematic of the cross-raster scan pattern applied in the multi-layer EBAM thermal analysis. The University of Alabama-Mechanical Engineering 11
  • 12. 4. Thermo-mechanical analysis Fig. 10 the simulated residual stress profile comparison Fig. 9 the simulated temperature contour comparison Fig. 11 the simulated residual stress distribution comparison The University of Alabama-Mechanical Engineering 12
  • 13. 4. Thermo-mechanical analysis Fig. 12 Simulated temperature fields and molten pool Fig. 13 Simulated temperature fields and molten pool geometry. geometry for raster scan: a) the temperature fields of layer-1; b) the cross sectional view of the field in a). The University of Alabama-Mechanical Engineering 13
  • 14. 4. Thermo-mechanical analysis Fig. 14 Simulated temperature history and thermal stress histories close the beam center starting point. Fig. 15 Simulated thermal stress fields of single straight scan just before cooling: a) Longitudinal stress; b) Transverse stress. The University of Alabama-Mechanical Engineering 14
  • 15. 4. Thermo-mechanical analysis Fig. 16 Simulated residual stress fields of single straight scan: a) Longitudinal stress; b) Transverse stress. The University of Alabama-Mechanical Engineering 15
  • 16. 4. Thermo-mechanical analysis Fig. 17 Simulated thermal stress and its cross sectional view. Fig. 18 Simulated thermal stress fields and their cross sectional views at the end of the 10 sec break between two sequential layers: a) Longitudinal stress; b) Transverse stress. The University of Alabama-Mechanical Engineering
  • 17. 4. Thermo-mechanical analysis Fig. 19 Simulated residual stress fields and their cross sectional views: a) Longitudinal stress; b) Transverse stress. Fig. 20 Simulated deformations (mm) for: a) Single straight scan; b) Multi-layer crossed raster scan. The University of Alabama-Mechanical Engineering
  • 18. 5. Conclusions • The raster scan pattern affects the temperatures and molten pool due to the residual heat from previous adjacent scan • Thermal stress histories on top (for both longitudinal and transverse) Compressive – just before beam coming; Tensile - solidified • Vertical thermal stress distribution (for both longitudinal and transverse) Tensile in solidified and the compressive just beneath the tensile • Vertical residual stress distribution (for both longitudinal and transverse) Max. tensile in solidified and it decreases to the compressive for a certain penetration. • The largest deformation follows the track of beam center The University of Alabama-Mechanical Engineering 18
  • 19. 6. Future work Fig. 21 Hatch melting The University of Alabama-Mechanical Engineering 19
  • 20. Acknowledgement Sponsor: NASA, No. NNX11AM11A Collaborator: Marshall Space Flight Center (Huntsville, AL), Advanced Manufacturing Team. The University of Alabama-Mechanical Engineering 20
  • 21. Q&A Thank you for your attention! Any Question? The University of Alabama-Mechanical Engineering 21
  • 22. Reference [1] Available from: http://www.arcam.com/. [2] Zaeh, M. F., and Lutzmann, S., 2010, "Modelling and simulation of electron beam melting," Production Engeering. Research and Development, 4, pp. 15-23. [3] Lampa, C., Kaplan, A. F. H., Powell, J., and Magnusson, C., 1997, "An analytical thermodynamic model of laser welding," Journal of Physics D: Applied Physics, 30(9), p. 1293. [4] Yang, J., Sun, S., Brandt, M., and Yan, W., 2010, "Experimental investigation and 3D finite element prediction of the heat affected zone during laser assisted machining of Ti6Al4V alloy," Journal of Materials Processing Technology, 210(15), pp. 2215-2222. [5] Liu, C., Wu, B., and Zhang, J., 2010, "Numerical Investigation of Residual Stress in Thick Titanium Alloy Plate Joined with Electron Beam Welding," Metallurgical and Materials Transactions B, 41(5), pp. 1129-1138. The University of Alabama-Mechanical Engineering 22