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- www.bcrc.be [email protected] Tél: 065/40 34 34
Predictive model applicable to water debindingof complex shape parts injection molded using
commercial feedstock
Vedi DupontC. Delmotte, J.P. Erauw, F. Cambier (1)
T. Boulanger, C. Emmerechts, B. Guerra, E. Beeckman (2)
(1) BCRC, Belgian Ceramic Research Centre4, Avenue Gouverneur Cornez, 7000 Mons, Belgium.
(2)SIRRIS12, rue Bois Saint Jean, 4102 Seraing, Belgium
BCERSFebuary 7 th 2011, Mons
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Contents
� Introduction
� Results and discussion
� Conclusion & perspectives
• CIM (Ceramic Injection Molding)• Definition of feedstocks• Goal & approach of the model
• Influence of temperature, and geometryduring a water debinding step
• Evolution of the microstructure • Influence of water debinding conditions on sintering behavior
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Ceramic Injection Molding
Industrial sector's concern : shaping of complex advanced ceramics parts- Selection of competitive forming method(s)- Low cost of processing and high end-product performance
CIM (CERAMIC INJECTION MOLDING) is more and more present on world markets.
Advantages : - Suited for the production of complex ceramic parts with precision , speed , and repeatability .- Less assembling and /or manipulation steps.
� 4 successive steps1. Plasticizing2. Injection3. Strengthening4. Ejection
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In the past: � formulation by ceramic producer
• Proportion powder-additives• Nature of binder & plasticizer• Nature of powder• Nature of adjuvants� Composition and behavior of feedstock clearly known
Today :� existence of commercial feedstocks• Ready-to-use• Composition unknown• No detailed technical data � Composition and behavior of commercial feedstocks "unknown"
What is a feedstock ?
BindersBinders
Ceramic Powder
Homogenization
Granulation
AdditivesAdditives
Feedstocks
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Disadvantage of CIM
Existence of a critical step :
Removal of the large amount of additives
Debindingmethods
Debindingmethods
Supercritical or catalytic debinding
Supercritical or catalytic debinding
Solvent debinding
Solvent debinding
Water debinding
Water debinding
- low cost- environmental friendly
Classicalthermal
debinding
Classicalthermal
debinding
Crucial step
� Several debinding methods of CIM parts
BCERSFebuary 7 th 2011, Mons 5
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Recommendations of the supplier :
� Debinding step- 24h in water(25°C)- thermal (HR : 20 to 2 °C / h)
� Sintering- 1600°C (HR : 130 °C / h)
Recommendations of the supplier :
� Debinding step- 24h in water(25°C)- thermal (HR : 20 to 2 °C / h)
� Sintering- 1600°C (HR : 130 °C / h)
80*20*5 mm3
Necessity to predict the time needed to remove a maximum fraction of the
soluble binder
As a function of geometry, temperature and immersion duration in water
Damaged partSwelling & Cracking
80*20*2 mm3
Sound part
Disadvantage of CIM
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Previous works
Lin & German :� For a infinite geometry, fraction of soluble binder remaining , Ln (1/F) = f (t)
with t immersion time
Shivashankar & German :� Extension of previous model for a finite geometry� Introduction of a new parameter : 1/Ψ (= S / V ) length scale
1
2
)1
ln( KtD
F+= 2ψ
π
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Goal & approach
Elaborate a predictive model of the water debinding of complex molded parts, to ease thermal post treatmen ts
Simple shapesParameters :
-Geometry
-Immersion time
-TemperatureElaboration of predictive model
Weight losses measured
Model validation Post-treatmentsReal complex shapes
Weight losses calculated
Weight losses measured
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Experimental procedure
� Preparation of samples- Injected at 160°C (Arburg 350-90 A270D), Alumina feedstock (Al2O3).- Debinded in stirred water at 25°, 40°et 55°C for varying immersion times.- Dried at 50°C during 48h .
Bars Cylinders
e (mm) 1.6 2.6 3.6 1 3 6
1/Ψ = S/V 1.477 0.997 0.748 2.250 0.917 0.583
60x10xe ∅16xe
Simple shapes Real complex shapes
Heat sink Nozzle
1/Ψ = 0.731 1/Ψ = 0.822
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Wide range of the length scale
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Results and discussion
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Influence of the temperature
Fraction of soluble binder remaining in the green (F) is expressed by :
*
•S.T.Lin, R.M.German, PMI vol 21 n° 5, 1989, pp 19-24.
With Ψ = V / S
1
2
)1
ln( KtD
F+= 2ψ
π
� Estimation of maximum weight loss in water :
W max (feedstock) ~ 6 %
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0
0,2
0,4
0,6
0,8
1
1,2
0 5 10 15 20 25 30
Ln(1
/F)
t/Ψ2 (h.mm -2)
Plot of Ln(1/F) against t/Ψ2 at different temperatures : Al2O3
(1/Ψ = 0.748)
25 °C
40 °C
55 °C
BCERSFebuary 7 th 2011, Mons 11
Influence of the temperature
25°C40°C55°C
0
0,2
0,4
0,6
0,8
1
1,2
0 5 10 15 20 25 30
Ln(1
/F)
t/Ψ2 (h.mm -2)
Plot of Ln(1/F) against t/Ψ2 at different temperatures : Al2O3
(1/Ψ = 0.748)
Diffusion controlled stage
Dissolution controlled stage
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0
0,2
0,4
0,6
0,8
1
1,2
0 5 10 15 20 25 30
Ln(1
/F)
t/Ψ2 (h.mm -2)
Plot of Ln(1/F) against t/Ψ2 at different temperatures : Al2O3
(1/Ψ = 0.748)
25 °C
40 °C
55 °C
BCERSFebuary 7 th 2011, Mons 11
Influence of the temperature
25°C40°C55°C
0
0,2
0,4
0,6
0,8
1
1,2
0 5 10 15 20 25 30
Ln(1
/F)
t/Ψ2 (h.mm -2)
Plot of Ln(1/F) against t/Ψ2 at different temperatures : Al2O3
(1/Ψ = 0.748)
Diffusion controlled stage
Dissolution controlled stage
0
0,2
0,4
0,6
0,8
1
1,2
0 5 10 15 20 25 30
Ln(1
/F)
t/Ψ2 (h.mm -2)
Plot of Ln(1/F) against t/Ψ2 at different temperatures : Al2O3
(1/Ψ = 0.748)
25°C40°C55°C
Diffusion controlled stage
Dissolution controlled stage
� 2 stages observed :
1. Dissolution controlled stage
�Binder just near the sample surface can dissolve quickly.
R limiting : Dissolution of binder at binder water interface.
2. Diffusion controlled stage
�Binder water interface moves inwards in the sample. Creation of a porous network within the green body.
R limiting : Diffusion of the solutes in the porous paths .
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• If 1 / Ψ (S / V) is high
Thin parts
Large contact surface between soluble binder and
solvent (water)
Kinetic of binder extraction is faster
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Influence of the geometry
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y = 0,0219x + 0,2338
0
0,2
0,4
0,6
0,8
1
1,2
1,4
0 10 20 30 40 50
Ln(1
/F)
t/Ψ2 (h.mm -2)
Plot of Ln(1/F) against t/ Ψ2 for different values of 1/ Ψ : Al 2O3 at 40 C : Diffusion controlled stage
� Diffusion controlled stage (T = 40°C)
� Inter-diffusion coefficient
Using the Shivashankar-German model,
1/Ψ range 0.583 - 0.917
Inter-diffusion coefD (cm2.s-1 )
6.16.10-5
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Influence of the geometry
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)exp(0 TR
EDD act−=
� Inter-diffusion coefficient D :follows an Arrhenius law
Diffusion controlled stage
Temperatures D (cm2.s-1)
25°C 4,92.10-5
40°C 6,16.10-5
55°C 6,61.10-5
Stage D0 (cm2.s-1) Eact (KJ.mol-1)
Diffusion 1.65.10-3 8.38
2 K t)( f )1
( + ,Ψ ,Τ =F
Ln
)673,0.0028,0()t
).(8380
exp(.2-
5,94.10 )1
( −+2Ψ
.2
Π= TRTF
Ln
as observed K2 depends on temperature
K2 (T) = 0.0028 T – 0.673
Elaboration of predictive model
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Validation of the predictive model
Heat sink Nozzle
1/Ψ = 0.731 1/Ψ = 0.822
)673,0.0028,0()t
).(8380
exp(.2-
5,94.10 )1
( −+2Ψ
.2
Π= TRTF
Ln
BCERSFebuary 7 th 2011, Mons 15
0
0,2
0,4
0,6
0,8
1
1,2
1,4
1,6
0 10 20 30 40 50 60 70
Ln (
1/F)
Immersion time (h)
theorical model - 0.822 - Nozzle
experimental points
0
0,2
0,4
0,6
0,8
1
1,2
1,4
0 10 20 30 40 50 60 70
Ln (
1/F)
Immersion time (h)
theorical model - 0.731 - Heat sink
experimental points
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5h, (1/Ψ = 1.477)
30 min 50 h
Cross section of specimens partially water debinded
at 40°C for 30 min & 50 h (1/Ψ = 0.748) .
The « Shrinking Core » can be clearly observed
Cross section of specimens partially water debinded
at 40°C for 30 min & 50 h (1/Ψ = 0.748) .
The « Shrinking Core » can be clearly observed
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Microstructure evolution
1
2
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SpecimensApparent
density(g/cm³)
1/FDensity
(supplier's data)
(g/cm³)
1h / 40°/ 3.6 3.61 1.13
3.94
1h / 40°/ 2.6 3.68 1.19
1h / 40°/ 1.6 3.80 1.29
50h / 40°/ 3.6 3.88 2.38
50h / 40°/ 2.6 3.93 3.70
50h / 40°/ 1.6 3.93 11.1
Sintering behavior
• Water debinding at 40°C for 1 and 50 h• Thermal debinding ( HR : 1 °C / min )
• Sintering at 1600°C ( HR : 2°C / min ) for 2 h
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e=2.6 mm
e=2.6 mm
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Conclusion
� The water debinding process depends on :
�the immersion time t �the longer the immersion time t, the larger the amount of removed soluble binder
� the temperature T� evolution of dissolution and diffusion coefficient
�the length scale (1 / Ψ) � the higher the length scale (1 / Ψ) , the shorter the immersion time needed
� Existence of two stages :
� Dissolution controlled / Diffusion controlled
� Creation of an interconnected porous network, facilitating subsequent thermal extraction of the insoluble binder
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Conclusion
)673,0.0028,0()t
).(8380
exp(.2-
5,94.10 )1
( −+2Ψ
.2
Π= TRTF
Ln
� Elaboration & validation of the predictive model :
� Sintering (preliminary) of simple specimens :
� 1/F < 1/F│limit → damaged parts
� 1/F > 1/F│limit → sound parts (d = 3.93 g/cm³)
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Methodology applicable to any kind of feedstocks
Methodology applicable to any kind of feedstocks
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Perspectives
� Optimize the thermal debinding step depending on this previous value (1/F)
� Estimate the minimal value of fraction of soluble binder remaining in the green (1/F) to obtain sound parts irrespective of geometry
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Acknowledgement
We thank the DGO6 of the “Service public de Walloni e” for its financial support (grant number 0716715).
We thank the DGO6 of the “Service public de Walloni e” for its financial support (grant number 0716715).
My colleagues
Cathy DelmotteJean-Pierre Erauw
My colleagues
Cathy DelmotteJean-Pierre Erauw
BCERSFebuary 7 th 2011, Mons 21
SIRRIS team
T. Boulanger, C. Emmerechts, B. Guerra, E. Beeckman
SIRRIS team
T. Boulanger, C. Emmerechts, B. Guerra, E. Beeckman
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Questions
Thank you for your attention
BCERSFebuary 7 th 2011, Mons 22