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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 215
“Mathematical Modeling And Numerical Simulation Of Selective Laser
Sintering By Considering Heat Transfer Process”
Prof. Vivekkumar J. Bharti1, Prof. Santosh R. Wankhade2, Prof. Yogesh S. Idhol3,
Prof. Savita J. patil4
1M.E. Student of College of Yadavrao Tasgaonkar Institute of Engineering &Technology[YTIET]
2HOD of Mechanical Department [YTIET]
3,4Assistant Professor, Mechanical Department [YTIET]
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract - Selective Laser Sintering (SLS) is an important
branch of Additive manufacturing (“3D printing”)
technologies. It is also know as leading process for
developing rapid prototype objects by selectively fusing
layers of powder according to numerically defined cross
sectional geometry. This process was initially developed to
produce polymer-based components, but due to the
advancement this process is now capable of producing
structurally perfect parts directly from metal powders. In
this manufacturing technique a pre-heated layer of material
powder undergoes a laser radiationina selective waysothat
three dimensional metallic or polymeric solid parts can be
produced.
In the present paper we use three dimensional steady and
transient finite element model developed in abaqus tostudy
the heat distribution taking place during sls process applied
to polycarbonate powder.
Key Words: SLS , Abaqus, Polycarbonate powder.
1. INTRODUCTION
The ever increasing competition in the world market for
manufactured products , development of new frontiers
demanding highly customized products in shortest possible
time has ultimately lead to thedevelopmentofnewmethods
of manufacturing whichhave abilitytochallengethe position
of conventional manufacturing.
Layered Manufacturing (LM), Additive Manufacturing
(AM) or Solid Freeform Fabrication (SFF) is a class of
manufacturing methods that has seen a rapid growth over
the years since in late 80’s. It enables quick production of
complex three-dimensional parts of designed macro and
microstructure directly from CAD data, completely
eliminating the intermediate tooling steps, therefore
shortening production time and reducing associated costs.
The invention of layered manufacturing has brought a
breakthrough in manufacturing technology because of
immense benefits associated withit. Additivemanufacturing
processes take the information from a computer-aided
design (CAD) file that is later converted to a
stereolithography (STL) file. In this process, the drawing
which are made in the CAD software is approximated by
triangles and sliced containing the information of each layer
that is going to be printed. Studies are reviewed whichwere
about the strength of products made in additive
manufacturing processes.However,thereisstill a lotofwork
and research to be accomplished before additive
manufacturing technologies become standard in the
manufacturing industry because not every commonly used
manufacturing material can be handled. The accuracyneeds
improvement to eliminate the necessity of a finishing
process. The continuous and increasing growth experienced
since the early days and the successful results up to the
present time allow for optimismthatadditivemanufacturing
has a significant place in the future of manufacturing.
The proposed work deals with sintering of polycarbonate
powder in which the mathematical modelingofdifferent sub
model such as optical, thermal and sintering have been
carried out. A transient three dimensional finite element
model is developed to simulate the phase transformation
during the selective laser sintering process. Owing to the
continuous movement ofthe laserbeamthemodel takesalso
into account the transient nature oftheproblem. Resultsfor
heat flux distributionusing polycarbonatepowderforsteady
and transient condition, will be presented.
2. MODELING
The physical processes which are mainlyassociatedwith the
SLS process are heat transfer and sintering of powder. The
modelling and numerical simulation of the SLS process
includes optical, thermal and rheological(sintering)
processes.
1.1 Sintering model :
The sintering behaviour commonly referred to the phase
transformation of the material from the powder state to the
solid state by the sintering process.
where ρ is the powder density, ρ max is the density of the
totally sintered (solidified) material, E is the activity energy
set at a correct value to obtain a good kinetics of the
sintering with referencetostandardprocessparametersand
with A the pre-exponential factor been fixedat8.84×1016 s–
1.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 216
1.2 Optical model :
The optical behavior is commonly referred to the
interactions between the laser beam and the powder bed
surface. Phenomena considered in the optical model are
reflection, transmissions, absorption, etc.
Where R is the reflectivity of the surface of the material, the
reflectivity of the CO2 laser in polycarbonate powder is
approximately 4% . I0 is the maximum beam intensity,
calculated from the laser power P and the characteristic
radius of the laser intensity profile w given as
where w is the characteristic radius, a function of the laser
radius, and P the laser power.
1.3 Thermal model :
The thermal behavior refers to the heat transfer
mechanisms that occur due to the laser light penetratingthe
powder bed. Phenomena considered in the thermal model
are conduction, convection and radiation.
is the heat equation with temperature- and sintering
dependent heat conduction properties (cp been the specific
heat and r the internal, volume, heat source term).
Heat conductivity:
The local effective heat conductivity, ke , relates not only to
the local temperature of the powdered bed, but also to the
heat conductivity of solid material ks , the heat conductivity
of air kg and the porosity Ɛ . A model to calculate the heat
conductivity is separately proposed by two conditions,low-
temperature and high-temperature. At low-temperature,
only the phenomenon of convection affects the heat
conductivity. While at high-temperature,theheattransferby
radiation is evidently enhanced that can also affect the heat
conductivity:
Where Φ is a model parameter function of the material
porosity Ɛ , and Dp is the average diameter of powdergrain.
The model parameters hrs and hrv are the radiation heat
transfer coefficients between solid surface of the powder
grain, and between voids respectively.
Specific heat:
The specific heat ofpolycarbonatematerial isassumedlinear
function of temperature in both the solid and the melt
phases. The temperature dependence of the specificheat, Cp
, is given by the following equation
The current FE approach relies on the geometrical
approximation of the powder bed by a 3D rectangular
parallelepiped mesh of 5mm x 0.8mm x 0.2mm for the
polycarbonate model. These mesh size are adapted to the
modeled laser trajectory so that it contain “DC3D8” in the
thermal FE analysis undertaken within the ABAQUS code.
Table -1: Material properties and process parameters for
the polycarbonate SLS
Property or
process
parameter
Full name Value Unit
Tinitial
Pre-heating
temperature
373 K
ρo
Initial density of
powder
600 Kg/m3
ρ
Full dense solid
material density
1200 Kg/m3
h Film coefficient 25 W/m2k
Ɛ Emissivity 0.8 -
E Activation energy 149.7 kJ/mol
K Conductivity 0.22 W/mk
Cp
Specific heat
capacity
1200 J/kgk
3. RESULT
Fig.1. Steady state condition
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 217
0.00E+00
2.00E-14
4.00E-14
6.00E-14
8.00E-14
1.00E-13
1.20E-13
1.40E-13
0 2 4 6
Heatflux
Time distance along path
Fig. 2 Time distance along path
Fig.3 Transient state condition
Fig. 4 Time distance along path
4. CONCLUSIONS
In this paper, we present the thermal modeling by finite
element method of a Selective Laser Sintering (SLS)process.
We model the behavior of the materials under this process
using three different sub-models: a sintering sub-model, an
optical sub-model, and the thermal sub-model.
Interpretation of the results both in terms of steady and
transient condition shows that the distribution of heat flux
fluctuate more in steady condition than in transient
condition.
Two cases of SLS processes are reported here: steady and
transient state, In the case of transient SLS, the modeling
approach was compared to experiments and showed a good
correspondence between the two.
REFERENCES
1. Lin Dong a, Ahmed Makradi b, Said Ahzi c and Yves
Remond d, ‘ Finite element analysis of temperature and
density distributions in selective laser sintering
process’, Materials Science Forum Vol. 553 (2007) pp
75-80online at http://www.scientific.net© (2007)
Trans Tech Publications, Switzerland
2. Kai Zeng, Deepankar Pal, Brent Stucker , ‘A review of
thermal analysis methods in Laser Sintering and
Selective Laser Melting’.
3. L. Dong, A. Makradi, S. Ahzi, Y. Remond,’Three-
dimensional transient finite element analysis of the
selective laser sintering process’, 2008 Published by
Elsevier B.V. doi:10.1016/j.jmatprotec.2008.02.040
4. X. Jian, R.S. Rana, ‘Simulation of transient temperature
for mixture of two materials in the selective laser
sintering process’, IET Optoelectron., 2012, Vol. 6, Iss. 5,
pp. 237–241 doi: 10.1049/iet-opt.2011.0058
5. Rahul B. Patil, Vinod Yadava, ‘ Finite element analysis of
temperature distributioninsinglemetallic powderlayer
during metal laser sintering’, International Journal of
Machine Tools & Manufacture 47 (2007) 1069–1080
6. K.R. Bakshi, A. V. Mulay, ‘ A Review on Selective Laser
Sintering: A RapidPrototypingTechnology’IOSR Journal
of Mechanical & Civil Engineering (IOSRJMCE) e-ISSN:
2278-1684,p-ISSN: 2320-334X PP 53-57
www.iosrjournals.org
7. Lin Dong, Nicolas Barth, J.P.M. Correia1 and Said Ahzi1,‘
Modeling and Numerical Simulation of Selective Laser
Sintering’ 17th International Conference on Thermal,
Mechanical and Multi-Physics Simulation and
Experiments inMicroelectronicsandMicrosystems978-
1-5090-2106-2/16/ ©2016 IEEE 2016
8. Nikolay K. Tolochko,Maxim K. Arshinov,Andrey V.
Gusarov, Victor I.Titov, Tahar Laoui and Ludo Froyen,
‘Mechanisms of selective laser sintering and heat
transfer in Ti powder’, Rapid Prototyping Journal
Volume 9 · Number 5 · 2003 · pp. 314–326 q MCB UP
Limited · ISSN 1355-2546 DOI
10.1108/13552540310502211
9. John D. Williams and Carl R. Deckard, ‘Advances in
modeling the effects of selected parameters on the SLS
process, Rapid PrototypingJournal Volume4 ·Number2
· 1998 · pp. 90–100 © MCB University Press · ISSN
1355-2546
10. Ming-shen M. Sun, Joseph J. Beaman, ‘ A Three
Dimensional Model for Selective Laser Sintering’.

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Mathematical Modeling and Numerical Simulation of Selective Laser Sintering by Considering Heat Transfer Process

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 215 “Mathematical Modeling And Numerical Simulation Of Selective Laser Sintering By Considering Heat Transfer Process” Prof. Vivekkumar J. Bharti1, Prof. Santosh R. Wankhade2, Prof. Yogesh S. Idhol3, Prof. Savita J. patil4 1M.E. Student of College of Yadavrao Tasgaonkar Institute of Engineering &Technology[YTIET] 2HOD of Mechanical Department [YTIET] 3,4Assistant Professor, Mechanical Department [YTIET] ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - Selective Laser Sintering (SLS) is an important branch of Additive manufacturing (“3D printing”) technologies. It is also know as leading process for developing rapid prototype objects by selectively fusing layers of powder according to numerically defined cross sectional geometry. This process was initially developed to produce polymer-based components, but due to the advancement this process is now capable of producing structurally perfect parts directly from metal powders. In this manufacturing technique a pre-heated layer of material powder undergoes a laser radiationina selective waysothat three dimensional metallic or polymeric solid parts can be produced. In the present paper we use three dimensional steady and transient finite element model developed in abaqus tostudy the heat distribution taking place during sls process applied to polycarbonate powder. Key Words: SLS , Abaqus, Polycarbonate powder. 1. INTRODUCTION The ever increasing competition in the world market for manufactured products , development of new frontiers demanding highly customized products in shortest possible time has ultimately lead to thedevelopmentofnewmethods of manufacturing whichhave abilitytochallengethe position of conventional manufacturing. Layered Manufacturing (LM), Additive Manufacturing (AM) or Solid Freeform Fabrication (SFF) is a class of manufacturing methods that has seen a rapid growth over the years since in late 80’s. It enables quick production of complex three-dimensional parts of designed macro and microstructure directly from CAD data, completely eliminating the intermediate tooling steps, therefore shortening production time and reducing associated costs. The invention of layered manufacturing has brought a breakthrough in manufacturing technology because of immense benefits associated withit. Additivemanufacturing processes take the information from a computer-aided design (CAD) file that is later converted to a stereolithography (STL) file. In this process, the drawing which are made in the CAD software is approximated by triangles and sliced containing the information of each layer that is going to be printed. Studies are reviewed whichwere about the strength of products made in additive manufacturing processes.However,thereisstill a lotofwork and research to be accomplished before additive manufacturing technologies become standard in the manufacturing industry because not every commonly used manufacturing material can be handled. The accuracyneeds improvement to eliminate the necessity of a finishing process. The continuous and increasing growth experienced since the early days and the successful results up to the present time allow for optimismthatadditivemanufacturing has a significant place in the future of manufacturing. The proposed work deals with sintering of polycarbonate powder in which the mathematical modelingofdifferent sub model such as optical, thermal and sintering have been carried out. A transient three dimensional finite element model is developed to simulate the phase transformation during the selective laser sintering process. Owing to the continuous movement ofthe laserbeamthemodel takesalso into account the transient nature oftheproblem. Resultsfor heat flux distributionusing polycarbonatepowderforsteady and transient condition, will be presented. 2. MODELING The physical processes which are mainlyassociatedwith the SLS process are heat transfer and sintering of powder. The modelling and numerical simulation of the SLS process includes optical, thermal and rheological(sintering) processes. 1.1 Sintering model : The sintering behaviour commonly referred to the phase transformation of the material from the powder state to the solid state by the sintering process. where ρ is the powder density, ρ max is the density of the totally sintered (solidified) material, E is the activity energy set at a correct value to obtain a good kinetics of the sintering with referencetostandardprocessparametersand with A the pre-exponential factor been fixedat8.84×1016 s– 1.
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 216 1.2 Optical model : The optical behavior is commonly referred to the interactions between the laser beam and the powder bed surface. Phenomena considered in the optical model are reflection, transmissions, absorption, etc. Where R is the reflectivity of the surface of the material, the reflectivity of the CO2 laser in polycarbonate powder is approximately 4% . I0 is the maximum beam intensity, calculated from the laser power P and the characteristic radius of the laser intensity profile w given as where w is the characteristic radius, a function of the laser radius, and P the laser power. 1.3 Thermal model : The thermal behavior refers to the heat transfer mechanisms that occur due to the laser light penetratingthe powder bed. Phenomena considered in the thermal model are conduction, convection and radiation. is the heat equation with temperature- and sintering dependent heat conduction properties (cp been the specific heat and r the internal, volume, heat source term). Heat conductivity: The local effective heat conductivity, ke , relates not only to the local temperature of the powdered bed, but also to the heat conductivity of solid material ks , the heat conductivity of air kg and the porosity Ɛ . A model to calculate the heat conductivity is separately proposed by two conditions,low- temperature and high-temperature. At low-temperature, only the phenomenon of convection affects the heat conductivity. While at high-temperature,theheattransferby radiation is evidently enhanced that can also affect the heat conductivity: Where Φ is a model parameter function of the material porosity Ɛ , and Dp is the average diameter of powdergrain. The model parameters hrs and hrv are the radiation heat transfer coefficients between solid surface of the powder grain, and between voids respectively. Specific heat: The specific heat ofpolycarbonatematerial isassumedlinear function of temperature in both the solid and the melt phases. The temperature dependence of the specificheat, Cp , is given by the following equation The current FE approach relies on the geometrical approximation of the powder bed by a 3D rectangular parallelepiped mesh of 5mm x 0.8mm x 0.2mm for the polycarbonate model. These mesh size are adapted to the modeled laser trajectory so that it contain “DC3D8” in the thermal FE analysis undertaken within the ABAQUS code. Table -1: Material properties and process parameters for the polycarbonate SLS Property or process parameter Full name Value Unit Tinitial Pre-heating temperature 373 K ρo Initial density of powder 600 Kg/m3 ρ Full dense solid material density 1200 Kg/m3 h Film coefficient 25 W/m2k Ɛ Emissivity 0.8 - E Activation energy 149.7 kJ/mol K Conductivity 0.22 W/mk Cp Specific heat capacity 1200 J/kgk 3. RESULT Fig.1. Steady state condition
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 217 0.00E+00 2.00E-14 4.00E-14 6.00E-14 8.00E-14 1.00E-13 1.20E-13 1.40E-13 0 2 4 6 Heatflux Time distance along path Fig. 2 Time distance along path Fig.3 Transient state condition Fig. 4 Time distance along path 4. CONCLUSIONS In this paper, we present the thermal modeling by finite element method of a Selective Laser Sintering (SLS)process. We model the behavior of the materials under this process using three different sub-models: a sintering sub-model, an optical sub-model, and the thermal sub-model. Interpretation of the results both in terms of steady and transient condition shows that the distribution of heat flux fluctuate more in steady condition than in transient condition. Two cases of SLS processes are reported here: steady and transient state, In the case of transient SLS, the modeling approach was compared to experiments and showed a good correspondence between the two. REFERENCES 1. Lin Dong a, Ahmed Makradi b, Said Ahzi c and Yves Remond d, ‘ Finite element analysis of temperature and density distributions in selective laser sintering process’, Materials Science Forum Vol. 553 (2007) pp 75-80online at http://www.scientific.net© (2007) Trans Tech Publications, Switzerland 2. Kai Zeng, Deepankar Pal, Brent Stucker , ‘A review of thermal analysis methods in Laser Sintering and Selective Laser Melting’. 3. L. Dong, A. Makradi, S. Ahzi, Y. Remond,’Three- dimensional transient finite element analysis of the selective laser sintering process’, 2008 Published by Elsevier B.V. doi:10.1016/j.jmatprotec.2008.02.040 4. X. Jian, R.S. Rana, ‘Simulation of transient temperature for mixture of two materials in the selective laser sintering process’, IET Optoelectron., 2012, Vol. 6, Iss. 5, pp. 237–241 doi: 10.1049/iet-opt.2011.0058 5. Rahul B. Patil, Vinod Yadava, ‘ Finite element analysis of temperature distributioninsinglemetallic powderlayer during metal laser sintering’, International Journal of Machine Tools & Manufacture 47 (2007) 1069–1080 6. K.R. Bakshi, A. V. Mulay, ‘ A Review on Selective Laser Sintering: A RapidPrototypingTechnology’IOSR Journal of Mechanical & Civil Engineering (IOSRJMCE) e-ISSN: 2278-1684,p-ISSN: 2320-334X PP 53-57 www.iosrjournals.org 7. Lin Dong, Nicolas Barth, J.P.M. Correia1 and Said Ahzi1,‘ Modeling and Numerical Simulation of Selective Laser Sintering’ 17th International Conference on Thermal, Mechanical and Multi-Physics Simulation and Experiments inMicroelectronicsandMicrosystems978- 1-5090-2106-2/16/ ©2016 IEEE 2016 8. Nikolay K. Tolochko,Maxim K. Arshinov,Andrey V. Gusarov, Victor I.Titov, Tahar Laoui and Ludo Froyen, ‘Mechanisms of selective laser sintering and heat transfer in Ti powder’, Rapid Prototyping Journal Volume 9 · Number 5 · 2003 · pp. 314–326 q MCB UP Limited · ISSN 1355-2546 DOI 10.1108/13552540310502211 9. John D. Williams and Carl R. Deckard, ‘Advances in modeling the effects of selected parameters on the SLS process, Rapid PrototypingJournal Volume4 ·Number2 · 1998 · pp. 90–100 © MCB University Press · ISSN 1355-2546 10. Ming-shen M. Sun, Joseph J. Beaman, ‘ A Three Dimensional Model for Selective Laser Sintering’.