0305 Olevsky - Theory of Sintering
-
Upload
khadijah-farid -
Category
Documents
-
view
229 -
download
0
Transcript of 0305 Olevsky - Theory of Sintering
-
7/27/2019 0305 Olevsky - Theory of Sintering
1/64
SINTERING THEORY
BRIEF INTRODUCTION
BY
EUGENE A. OLEVSKY
SAN DIEGO STATE UNIVERSITY, CALIFORNIA, USA
2011 FAST
Spring School
-
7/27/2019 0305 Olevsky - Theory of Sintering
2/64
1. Science of Sintering: Fundamentals and
Historical Development
2. Classical Models of Sintering: Viscous and
Diffusion Mechanisms of Mass Transport
3. Continuum Modeling of Powder Consolidation
4. Multi-Scale Modeling of Sintering5. Extrapolation of Sintering Concepts Towards
Constitutive Modeling of SPS
6. Sample SPS Problem Solutions
7. Further prospects of sintering modeling
SUMMARY
-
7/27/2019 0305 Olevsky - Theory of Sintering
3/64
1. Science of Sintering: Fundamentals and
Historical Development
2. Classical Models of Sintering: Viscous and
Diffusion Mechanisms of Mass Transport
3. Continuum Modeling of Powder Consolidation
4. Multi-Scale Modeling of Sintering5. Extrapolation of Sintering Concepts Towards
Constitutive Modeling of SPS
6. Sample SPS Problem Solutions
7. Further prospects of sintering modeling
SUMMARY
-
7/27/2019 0305 Olevsky - Theory of Sintering
4/64
PHYSICAL BASIS OF SINTERING
50 years to find out!
Surface tension phenomena
-
7/27/2019 0305 Olevsky - Theory of Sintering
5/64
PHYSICAL BASIS OF SINTERING
Surface tension phenomena
-
7/27/2019 0305 Olevsky - Theory of Sintering
6/64
-
7/27/2019 0305 Olevsky - Theory of Sintering
7/64
-
7/27/2019 0305 Olevsky - Theory of Sintering
8/64
-
7/27/2019 0305 Olevsky - Theory of Sintering
9/64
-
7/27/2019 0305 Olevsky - Theory of Sintering
10/64
Frenkel approach (1945) Pines approach (1946)
pore(vacancies)
coalescence of viscous particles
driven by surface tension
C Co 12
r
kT
V2t
E 2s
evaporation of emptiness
SINTERING THEORY
-
7/27/2019 0305 Olevsky - Theory of Sintering
11/64
1. Science of Sintering: Fundamentals and
Historical Development
2. Classical Models of Sintering: Viscous and
Diffusion Mechanisms of Mass Transport
3. Continuum Modeling of Powder Consolidation
4. Multi-Scale Modeling of Sintering5. Extrapolation of Sintering Concepts Towards
Constitutive Modeling of SPS
6. Sample SPS Problem Solutions
7. Further prospects of sintering modeling
SUMMARY
-
7/27/2019 0305 Olevsky - Theory of Sintering
12/64
Mass Transport in Sintering
From Swinkels and Ashby
-
7/27/2019 0305 Olevsky - Theory of Sintering
13/64
Ashby Sintering Maps
-
7/27/2019 0305 Olevsky - Theory of Sintering
14/64
COMPLEX SHAPE PARTS PRODUCED VIA
POWDER METALLURGY ROUTE
flange pulley
palate expander parts foldable paper hole punch
metal fiber filter for
airbag inflators
auto transmission sprockets
camshaft sprocket
-
7/27/2019 0305 Olevsky - Theory of Sintering
15/64
It was necessary to combine ideas of
MECHANICS
&
MATERIALS SCIENCE
The breakthrough happened in the end of 1980s
Theory of Sintering: Practical Implementation
-
7/27/2019 0305 Olevsky - Theory of Sintering
16/64
1. Science of Sintering: Fundamentals and
Historical Development
2. Classical Models of Sintering: Viscous and
Diffusion Mechanisms of Mass Transport
3. Continuum Modeling of Powder Consolidation
4. Multi-Scale Modeling of Sintering5. Extrapolation of Sintering Concepts Towards
Constitutive Modeling of SPS
6. Sample SPS Problem Solutions
7. Further prospects of sintering modeling
SUMMARY
-
7/27/2019 0305 Olevsky - Theory of Sintering
17/64
The Main Constitutive Relationship
( ) 1
3ij ij ij L ij
We e P
W
externally applied material resistance sinteringstresses
Generalized
viscosity:
corresponds to the
constitutive properties of
particle material
Effective sintering stress:
function of porosity
Strain rate component
Bulk modulus:
Resistance to the volume change
function of porosity
Shear modulus:
Resistance to the shape change
function of porosity
Volume strain rate
Olevsky E.A. (1998), Theory of sintering: from discrete to continuum. Review,Mater. Sci. & Eng. R: Reports, 40-100
-
7/27/2019 0305 Olevsky - Theory of Sintering
18/64
Continuum Theory of Sintering
( ) 1[ ( ) ]
3ij ij ij
we
w
ij
Without considering sintering stress
is the ij component of the stress tensor;
0( ) 2w w
( )
( )
y
m
w
w Aw
Linear viscous (hot deformation of
amorphous materials; free sintering)
Plastic (cold pressing)
Power-law creep (hot deformation of
crystalline materials)
effective stress( )w
-
7/27/2019 0305 Olevsky - Theory of Sintering
19/64
3
2
2 (1 )
3
(1 )
( ) 1[ ( ) ]
3ij ij ij
we
w
Bulk modulus
Shear modulus
0 Shear viscosity of the fully-dense material
2 21
1w e
Equivalent effective
strain rate
11 22 33iie volume change rate
ij Kronecker delta
2 2 2
1 2 2 3 3 1
1( ) ( ) ( )
3
Shape change rate
Continuum Theory of Sintering
-
7/27/2019 0305 Olevsky - Theory of Sintering
20/64
Including sintering stress:
( ) 1[ ( ) ]
3ij ij ij l ij
we p
w
lp The effective sintering stress
Surface tension
ij external stressFor free sintering, no external stress, 0ij
2
0
3
(1 )2lp r
0r Radius of the particle
Continuum Theory of Sintering
-
7/27/2019 0305 Olevsky - Theory of Sintering
21/64
Problem of free sinter ing of a porous body
For linear viscous phase
( ) 10 [ ( ) ]3
ij ij ij l ijw e pw
Projection on r direction: (a)
0( ) 2w w
0
12 [ ( ) ]
3r le p
Projection on z direction: (b)01
2 [ ( ) ]3
z le p
(a)*2+(b)0
12 [ (2 ) 3( ) ] 3
3r z le p
0 02 2 3 3 2r z l l e e p p e
Continuity equation
1e
Continuum Theory of Sintering
-
7/27/2019 0305 Olevsky - Theory of Sintering
22/64
2
0
3
00
3
(1 )2
2 (1 )2 12
3
lp re
s :Specific time of sintering
1
0 0
9exp( )
8s sdt
r
0 0 0 0 0 0
9 9 9ln8 8 8
dtr r r
Continuum Theory of Sintering
P i i i id di d f i t i f d li d
-
7/27/2019 0305 Olevsky - Theory of Sintering
23/64
Pressing in rigid die and free sintering of a powder cylinder
E. Olevsky, G. Timmermans, M. Shtern, L. Froyen, and L. Delaey, The permeable element method for
modeling of deformation processes in porous and powder materials: Theoretical basis and checking byexperiments, Powd. Technol. - 93/2, 123-141 (1997)
-
7/27/2019 0305 Olevsky - Theory of Sintering
24/64
Gravity Influence: Grain Segregation Effect
E.A. Olevsky and R.M. German, Effect of gravity on dimensional change during sintering, II. Shape distortion,Acta Mater., 48, 1167-1180 (2000)
-
7/27/2019 0305 Olevsky - Theory of Sintering
25/64
1. Science of Sintering: Fundamentals and
Historical Development
2. Classical Models of Sintering: Viscous and
Diffusion Mechanisms of Mass Transport
3. Continuum Modeling of Powder Consolidation
4. Multi-Scale Modeling of Sintering5. Extrapolation of Sintering Concepts Towards
Constitutive Modeling of SPS
6. Sample SPS Problem Solutions
7. Further prospects of sintering modeling
SUMMARY
-
7/27/2019 0305 Olevsky - Theory of Sintering
26/64
Sintering theory was traditionally
developed either as the
application of complex diffusion
or viscous flow mechanisms to a
simple geometry or as complex
evolution of microstructure withsimple diffusion mechanisms. For
example, the bulk modulus can
be obtained from the solution of
the problem of hydrostatic
loading of the chosenrepresentative unit cell. The
disadvantage of this model basis
is the high degree of the
idealization of the grain-pore
structure.
MULTI-SCALE MODELING OF SINTERING
Idealized unit-cell used for the
determination
of the effective constitutive parameters
strainvolume
stresschydrostati~
-
7/27/2019 0305 Olevsky - Theory of Sintering
27/64
Normalized shear modulus Normalized bulk modulus
Kuhn & Downey 2
3(2 (1 )2)(1 )
2
9(2 )(1 )
for Green 2
3
(1 1/3 )2
(3 21/ 4)(1 )
8
9
(1 1/ 3) 2 ln 2
(3 21/4)(1 )
plastic Shima & Oyane 2
9(1 )4
2
3
(1 )9
2.49 0 .514
flow Doraivelu et al.2(2(1 )2 1)
3(2 (1 )2)(1 )
2(2(1 )2 1)
9(2 )(1 )
Skorohod (1 )2
2
3
(1 )3
Gurson (Doraivelu et al.
approximation)
2
9
1 3
1 2
2
9
1 3
1 21
2
for Ponte Castaneda (1 )2 / ( m 1 )
1 2 3
27(1 )2 ( m 1 )
8
power-law Cocks (1 )2 / ( m 1 )
1 2 3
(m 1)(1 )(1 )2 ( m 1 )
3
creep Duva & Crow (1 )2 / ( m 1 )
1 2 3
2
3
1 m
mm
2 (m 1)
(m is thecreep
exponent)
McMeeking & Sofronis 1
1
2 (m1)
2
3
1 m
mm
2 (m 1)
CONSTITUTIVE PARAMETERS OF MODELS FOR POROUS
MATERIAL DENSIFICATION
-
7/27/2019 0305 Olevsky - Theory of Sintering
28/64
grain growthchange pixel color
We use a digitized microstructure
pore migrationswap pixels
Monte Carlo Model was used to simulate grain growth,
vacancy diffusion and vacancy annihilation
vacancy annihilationmove pixel out
N
i j
ji qqE1
8
1
,12
1Energy
E. Olevsky, V. Tikare, and T. Garino, Multi-scale modeling of sinteringA Review,J. Amer. Ceram. Soc., 89 (6),1914-1922 (2006)
-
7/27/2019 0305 Olevsky - Theory of Sintering
29/64
Mesoscale Simulation Using the Potts Model
E. Olevsky, V. Tikare, and T. Garino, Multi-scale
modeling of sintering A Review, J. Amer.
Ceram. Soc., 89 (6), 1914-1922 (2006)
E. A. Olevsky, B. Kushnarev, A. Maximenko, V.
Tikare, and M. Braginsky, Modeling anisotropic
sintering in nanocrystalline ceramics, Phil.
Mag., 85, 2123-2146 (2005)
V. Tikare, M. Braginsky, E. Olevsky, and D. L.
Johnson, Numerical simulation of anisotropic
shrinkage in a 2D compact of elongatedparticles, J. Amer. Ceram. Soc., 88, 1, 59-65
(2005)
M. Braginsky, V. Tikare, and E. Olevsky,
Numerical simulation of solid state sintering,
Int. J. Solids and Structures, 42, 621-636 (2005)
E. Olevsky, B. Kushnarev, A. Maximenko, and
V. Tikare, Modeling of sintering at multiplelength scales: anisotropy phenomena, TMS
Letters, 3, 55-56 (2004)
V. Tikare, M. Braginsky, and E.A. Olevsky,
Numerical simulation of solid-state sintering: I,
Sintering of three particles, J. Amer. Ceram.
Soc., 86, 49-53 (2003)
First publication:V. Tikare, E.A. Olevsky, and M.V. Braginsky,
Combined macro-meso scale modeling of
sintering, in: Recent Developments in Computer
Modeling of Powder Metallurgy Processes, ed. A.
Zavaliangos and A. Laptev, IOS Press, 85-104(2001)
-
7/27/2019 0305 Olevsky - Theory of Sintering
30/64
Results: Simulation of Microstructural Evolution during
Sintering
Time, t = 0 MCS t = 2,000 MCS t = 50,000 MCS
Digitized images can be mined for many types of data
Vacancy anihilation: jump and shift algorithms
-
7/27/2019 0305 Olevsky - Theory of Sintering
31/64
Diffusion mass
transport
Vacancy anihilation
Potts Model
Meso-Scale FEM
Macro-Scale FEM
Macroscopic shape distortions
Density distribution
Macroscopic damage
Macroscopic stress-strain state
Schematics of Multi-Scale Modeling
Two possible approaches:
Direct determination of the macroscopic constitutive
parameters based on the mesoscale simulations.
The macroscopic level envelopes the mesoscopic
simulators.
-
7/27/2019 0305 Olevsky - Theory of Sintering
32/64
CONSTITUTIVE PARAMETERS
sintering stress bulk and shear moduli grain growth kinetics
DETERMINATION
Theoretical:Mesoscale Simulation
Experimental:Sinter-forging and free
sintering experiments
Sintering Stress and Bulk Modulus Approximations
-
7/27/2019 0305 Olevsky - Theory of Sintering
33/64
d
c)1(
3
2
26.0L )1(7.1P
0
20
40
60
80
100
120
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35
Porosity
Bu
lkModulus
Normalized Bulk Modulus (Potts) Normalized Bulk Modulus (Skorohod)
Normalized Bulk Modulus (approx)
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
0.7 0.75 0.8 0.85 0.9 0.95
Relative Density
Sintering
Stres
s
Potts Model Approximation Skorohod Model
Sintering Stress and Bulk Modulus Approximations
Based on Mesoscale Simulations
bL )1(aP
12.1
23.2)1(
3
2
E. Olevsky, V. Tikare, and T. Garino, Multi-scale modeling of sinteringA Review,J. Amer. Ceram. Soc., 89 (6),1914-1922 (2006)
Multi-Scale Virtual Reality of Powder Processing
-
7/27/2019 0305 Olevsky - Theory of Sintering
34/64
Boundary conditions
initial state current state
each element
at each time step
Multi-Scale Virtual Reality of Powder Processing
-
7/27/2019 0305 Olevsky - Theory of Sintering
35/64
Sample problem solution: sintering with inclusion
-
7/27/2019 0305 Olevsky - Theory of Sintering
36/64
1. Science of Sintering: Fundamentals and
Historical Development2. Classical Models of Sintering: Viscous and
Diffusion Mechanisms of Mass Transport
3. Continuum Modeling of Powder Consolidation
4. Multi-Scale Modeling of Sintering5. Extrapolation of Sintering Concepts Towards
Constitutive Modeling of SPS
6. Sample SPS Problem Solutions
7. Further prospects of sintering modeling
SUMMARY
MODELING OF SPS
-
7/27/2019 0305 Olevsky - Theory of Sintering
37/64
Overwhelming majority of publications on SPS describe
empiric trial-and-error attempts to consolidate various
powder material systems.
The conducted theoretical studies are mostly reduced
to the modeling of temperature and electric current
density distributions. In practically all of the
publications the role of electrical field is narrowed downto the generation of Joule heat, which thereby reduces
the theoretical framework, required for the description
of shrinkage and grain growth, to the existing
constitutive models of powder consolidation.
Generic physically-based modeling concepts are
currently in strong demand to enable the understanding
and control of the thermal and field effects a
distinguishing set of factors rendering different spark-
plasma vs. conventional hot pressing and sinteringresults.
MODELING OF SPS
-
7/27/2019 0305 Olevsky - Theory of Sintering
38/64
Heating rate 20C/min
60
65
70
75
80
85
90
95
100
0 50 100 150 200 250 300 350 400 450
Temperature (C)
Relative
density(%)
FAST 450C-80 MPa
FAST 400C-149 MPa
FAST 350C- 229 MPa
HP 450C-80 MPa
HP 400C-275 MPa
HP 350C -460 MPa
Courtesy S. Kandukuri & L. Froyen
Comparative study of SPS HP of hypereutectic Al-Si-Fe-X powder
-
7/27/2019 0305 Olevsky - Theory of Sintering
39/64
electromigration
(diffusion enhancement)
electroplasticity
(electron wind,
magnetic depinning ofdislocations)
dielectric breakdown of
oxide films at grain
boundaries ponderomotive forces
pinch effect
surface plasmons
Field Effects in SPS
high heating rates
high local non-
uniformities of
temperature distribution
(local melting andsublimation)
macroscopic
temperature gradients
thermal diffusion
thermal stresses
Thermal Effects in SPS
SPS: ENHANCEMENT OF MASS TRANSPORT
-
7/27/2019 0305 Olevsky - Theory of Sintering
40/64
SPS: ENHANCEMENT OF MASS TRANSPORT
E. Olevsky and L. Froyen, Constitutive modeling of spark-plasma sintering of conductive
materials, Scrip ta Mater., 55, 1175-1178 (2006)
E. Olevsky, S. Kandukuri, and L. Froyen, Consolidation enhancement in spark-plasma sintering:
Impact of high heating rates, J. Ap p. Phys., 102, 114913-114924 (2007)
E. Olevsky and L. Froyen, Influence of thermal diffusion on spark-plasma sintering, J. Amer.Ceram. Soc., 92, S122-132 (2009)
electromigration(diffusion enhancement)
electroplasticity
(electron wind,
magnetic depinning of
dislocations) dielectric breakdown of
oxide films at grain
boundaries
ponderomotive forces
pinch effect surface plasmons
Field Effects in SPS
high heating rates high local non-
uniformities of
temperature distribution
(local melting and
sublimation) macroscopic
temperature gradients
thermal diffusion
thermal stresses
Thermal Effects in SPS
Mi h i l M d l
-
7/27/2019 0305 Olevsky - Theory of Sintering
41/64
Micromechanical Model
E. A. Olevsky, B. Kushnarev, A.
Maximenko, V. Tikare and M.
Braginsky, Modelling of
anisotropic sintering in crystalline
ceramics, Philosophical Magazine,
85, (19), 2123-2146 (2005)
2
p
a
p
cr
a
2
p
c
p
ar
c
2
1 2 3x x x xb y b y b
2
1 2 3y y y yb x b x b
0
sin
2
ap
xx
c cdx c
c
( ) ;xc
cr
0 0 0xx yy
22 33 1 1 3 3 1 1 3
sin sin2 2 2 2 2 2 2
x xx p p
c c
c c y c cc r c c c r c
where is the surface tension, is the dihedral angle, a and c
are the grain semi-axes; x - effective (far-field) external stress in
the x-direction (compressive x is negative). Parameter
px
c c
c
is a local stress on the grain boundary (
pc c
c
is the
stress concentration factor).
23 1 1
sin2
gb gb pxgbx
cp p
D c c
kT c r c c a a c c
gb gbgb xy
DJ
kT y
( )
2
gb
y
gbx
p p
J c
a a c c
gb
yJ is the flux of matter in the direction of the
axis ycaused by the grain boundary diffusion,
gbD is the coefficient of the grain boundary
diffusion,gb
is the grain boundary thickness,
k Boltzman constant; T absolutetemperature.
-
7/27/2019 0305 Olevsky - Theory of Sintering
42/64
Influence of High Heating Rates
Experimentally, it has been shown in a number of investigations that
an increase in heating rate considerably increases the consolidation
rate of conductive and non-conductive powders during SPS. For example, it was shown for an alumina powder (Zhou et al.) that
the increase of heating rate from 50 to 300C/min with the same
maximum temperature and the corresponding six time decrease of
sintering time allowed obtaining the same final density. Physically,
this was attempted to be explained as a result of the existence of
additional defects in the material directly related to high heating ratesand short time of the process. They could be initial biographic
defects resulting from processes of powder synthesis (Ivensen or
defects in grain-boundaries between particles (Dabhade et al.).
Gillia and Bouvard have conducted a series of fundamental
comparative experiments on sintering of WC-Co powder system with
different heating cycles. They employed cycles with the same average
heating rate but with various temperature histories (by employing
sequences of steady ramps and isothermal periods). Their results
indicate the dependence of the densification rate on the average
heating rate but no dependence on the temperature history.
-
7/27/2019 0305 Olevsky - Theory of Sintering
43/64
Influence of High Heating Rates
E. Olevsky, S. Kandukuri, and L. Froyen, Consolidation
enhancement in spark-plasma sintering: Impact of high
heating rates,J. App. Phys. 102, 114913-114924 (2007)
For an aluminum alloy
powder
, ,x gbx crx f G
4
22
4 2
31 1 1
8
s sD
kTG
x = e =
1-
3
1.3400fd GG G
G
G is the porous materials grain growth rate, 0fdG
is the grain growth rate of the fully-dense materialwith the grain size 0G , 0G is the initial grain size of
the porous (powder) material
Du and Cocks
4 16.67 10 3.55 10
0
fd fd TG G t
Beck et al. fdG is the current grain size of the fully-densematerial; 0
fdG is the initial grain size of the fully-
dense material; tis time, s; and Tis temperature, K
3
4 1.3400
1 235 /6.67 10 ln , 533
0, 533
GK sG if T K
G K G
if T K
dT
dt = constis the heating rate, K/s
Influence of High Heating Rates
-
7/27/2019 0305 Olevsky - Theory of Sintering
44/64
Influence of High Heating Rates
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0 1000 2000 3000
Time, s
Porosity
200C/min
100C/min
50C/min
25C/min
10C/min
For aluminum powder
Influence of High Heating Rates
-
7/27/2019 0305 Olevsky - Theory of Sintering
45/64
Influence of High Heating Rates
-4.E-03
-3.E-03
-2.E-03
-5.E-04
150 250 350 450 550
Temperature, C
ShrinkageRate,1
/s
200C/min
100C/min
50C/min
25C/min
10C/min
-7.E-03
-5.E-03
-3.E-03
-1.E-03
150 250 350 450 550
Temperature, C
ShrinkageR
ate,1/s
200 C/min
100 C/min
50 C/min
For aluminum powder
Model
Experiment
-
7/27/2019 0305 Olevsky - Theory of Sintering
46/64
Influence of Thermal Diffusion
J is the vacancy flux, D is the coefficient ofdiffusion, vC is the vacancy concentration,
vC is the vacancy concentration gradient,*Q is the heat of vacancy transport, T is thetemperature gradient.
*
v v
Q TJ D C C
kT T
Influence of Thermal Diffusion
-
7/27/2019 0305 Olevsky - Theory of Sintering
47/64
Influence of Thermal Diffusion Ludwig-Soret effect of thermal diffusion causes concentration gradients in
initially homogeneous two-component systems subjected to a temperature
gradient.
J. Chipman, The Soret effect, Journal of the American Chemical Society, 48, 2577-2589 (1926)
For the case of atomic and vacancy diffusion in crystalline solids, this effect
was studied by a number of authors including its theoretical interpretation by
Shewmon and Schottky.
P. Shewmon, Thermal diffusion of vacancies in zinc, Journal of Chemical Physics, 29, (5), 1032-1036 (1958)
G. Schottky, A theory of thermal diffusion based on lattice dynamics of a linear chain, Physica Status Solidi, 8, (1),
357 (1965)
For the electric-current assisted sintering, the effect of thermal diffusion wasanalyzed by Kornyushin and co-workers. Later, for rapid densification, the role
of temperature gradients was studied by Searcy and by Young and McPherson.
Y. V. Kornyushin, Influence of external magnetic and electric-fields on sintering, structure and properties, Journal of
Materials Science, 15, (3), 799-801 (1980)
A. W. Searcy, Theory for sintering in temperature-gradients - role of long-range mass-transport, Journal of the
American Ceramic Society, 70, (3), C61-C62 (1987)
R. M. Young and R. McPherson, Temperature-gradient-driven diffusion in rapid-rate sintering, Journal of theAmerican Ceramic Society, 72, (6), 1080 (1989)
Johnson argued against thermal diffusion significance in microwave sintering
D. L. Johnson, Microwave-heating of grain-boundaries in ceramics, Journal of the American Ceramic Society, 74, (4),
849-850 (1991)
We demonstrate a possible significance of thermal diffusion for SPSE. Olevsky and L. Froyen, Influence of thermal diffusion on spark-plasma sintering, J. Amer. Ceram. Soc. 92, S122-
132 (2009)
Influence of Thermal Diffusion
-
7/27/2019 0305 Olevsky - Theory of Sintering
48/64
ue ce o e us oJ is the vacancy flux, D is the coefficient ofdiffusion,
vC is the vacancy concentration,
vC is the vacancy concentration gradient,*
Q is the heat of vacancy transport, T is thetemperature gradient.
*
v v
Q TJ D C C
kT T
2v fC HC T
kT
*v fDC T
J H QkT T
*
m fQ H H
Schottky:
Young &McPherson:
Wirtz:
Kornyushin:
mH is the enthalpy of vacancy migration;
fH is the enthalpy of vacancy formation
vm
DC TJ H
kT T
;
v m f TT
C H HJ D T
k T T
did not include the term vC ! Otherwise:
T is the thermal diffusion ratio ( T is
the spatial average of temperature)
v mT
C H
k T We re-define:
TdivJ D T T
The driving force for
the vacancy migration:
T
TT q
dt
C
Heat transfer equation:
T is the thermal conductivity; C is
heat capacity; t is time; and q is the
heat production per unit volume of thematerial and per unit time, which in thecase of SPS can be represented as
2
eq E , where e is the specificelectric conductivity, and E is theelectric field intensity2T
e
T
TdivJ D E
T t
C
Influence of Thermal Diffusion
-
7/27/2019 0305 Olevsky - Theory of Sintering
49/64
22 2gb Ttd gb gb eT
TJ divJ G D E G
T t
C2T e
T
TdivJ D E
T t
C
2
2 2
2
gbgb gb Ttd td
gbx e
Tp p
DJ T GE
T tG r G r
C
_ ,gbx gbx
curvature driven th diffusion driven
x crx f G
x
= e =
1-
3
10 1.3401.5 10 /G
G m sG
E. Olevsky and L. Froyen, Influence of thermal diffusion on spark-plasma sintering, J. Amer. Ceram. Soc. 92, S122-132 (2009)
T is the thermal conductivity; C is
heat capacity; t is time; and q is the
heat production per unit volume of thematerial and per unit time, which in thecase of SPS can be represented as
2
eq E , where e is the specificelectric conductivity, and E is theelectric field intensity
is porosity; G is the average grain size
Influence of Thermal Diffusion
-
7/27/2019 0305 Olevsky - Theory of Sintering
50/64
25
125
225
325
425
525
625
0 200 400 600 800 1000
Time, s
Temperatu
re,C
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
Porosity
Temperature
Porosity - Model
Porosity - Experime nt
25
207
389
571
753
936
1118
1300
0 70 141 211 281 352 422
Time, s
Temperatu
re,
C
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
0.45
Porosity
Temperature
Porosity - Model
Porosity - Experiment
Porosity kinetics during SPS of aluminum
powder. Comparison of the developed model
taking into account the impact of thermal
diffusion with experimental data of Xie et al.,
Effect of interface behavior between particles on
properties of pure al powder compacts by spark
plasma sintering, Materials Transactions, 42, (9),1846-1849 (2001)
Porosity kinetics during SPS of alumina powder.
Comparison of the developed model taking into
account the impact of thermal diffusion with
experimental data of Shen et al., Spark plasma
sintering of alumina, J. Amer. Ceram. Soc., 85, (8),
1921 (2002)
3
2
11
2 223
4 24
0
2
2
2
3 32 129 2 23
1 4 1 9 1 2 exp 1
3 2
2 1
m
m m
xx
gb gb ref
gbx
cr
gb gb v m
e
T
G G
D G
QkTGA G
RT
D C H TE
t Gk T
C
curvature-driven grain boundary diffusion thermal diffusion power-law creep
Influence of Thermal Diffusion
-
7/27/2019 0305 Olevsky - Theory of Sintering
51/64
The intensity of thermal diffusion increases for
higher pulse frequencies.
The thermal diffusion promotes components
(atoms and vacancies) separation. At early stagesof sintering, this should lead to the growth of
inter-particle necks, which corresponds to the
enhancement of sintering. At the final stages of
sintering, however, the pores may serve as
vacancy sinks under thermal diffusionconditions, which impedes sintering.
It is possible that the increased pulse frequencies
enhance sintering at the early stages of SPS and
hinder sintering at the late stages of SPS
process. In some experimental studies the pulse frequency
was found to have a limited impact on SPS
results - its contributions at early and late stages
of SPS could offset each other.
TJ D TT
E. Olevsky and L. Froyen, Influence of thermal diffusion on spark-plasma sintering, J. Amer. Ceram. Soc. 92, S122-132 (2009)
Major Components of Densification-Contributing Mass
-
7/27/2019 0305 Olevsky - Theory of Sintering
52/64
Transfer During SPS (model including electromigration):
EC C J E
Nernst-Einstein equation
grain-boundary diffusion power-law creep
driving sources
externally applied load
sintering stress
electromigration
*gb gb
E q
D
C Z ekT
Blechs formula
gb gbD
CkT
where is the atomic volume, *Z is the valence of a migrating ion, and qe is
the electron charge (the product*
qZ e is called the effective charge).
*1gb gbgb xy q
D UJ Z e
kT l y
U and l are the electric potential and the characteristic length along theelectric field.
( )
2
gb
y
gbx
p
J c
ca a
*
2 2
3 1 1
2
gb gb q pxgbx
pp
D Z e G rU
kT l G r G GG r
is the surface tension, x - effective (far-field) external stress in the x-
direction
G a c is the grain size, p p pr a c is the pore radius.
M. Scherge, C.L. Bauer, and W.W. Mul l ins,
Acta Met. Mater., 43 (9), 3525-3538 (1995):
electromigration stress of 23MPa along grain
boundaries under an electric field of 500 V/m (in a 1-
thick film) and up to GPa range stresses for grain
structures with closed surface junctions
M.R. Gun go r and D. Marou das, Int. J. Fractur e,
109 (1), 47-68 (2001): electromigration stress of
140MPa in a 1 -thick film under the field of about 425
V/m
Q.F. Duan and Y.L. Shen , J. Appl . Phys . 87 (8),
4039-4041 (2000): electromigration stress of
450MPa along fast-diffusion length of 15 under 650
V/m
Z . Suo , Q . Ma, and W.K . Meyer , MRS
Symposi um Pr oceed in g s, 6p . (2000):
electromigration stress in 0.5 -thick Al film under 300V/m field should reach the level of 1.5GPa
C tit ti M d l f S k Pl Si t i
-
7/27/2019 0305 Olevsky - Theory of Sintering
53/64
5
2
1
3*
2 2
2 2
3 1 1 3 31 1
2 22
m
gb gb q p xx gbx cr x x
pp
D Z e G r UA
GkT l G r G G G r
G is the grain size; pr is the pore radius; A and m are power-law creep frequencyfactor and power-law creep exponent, respectively; gbD is the coefficient of the
grain boundary diffusion, gb is the grain boundary thickness, kis the Boltzmans
constant, T is the absolute temperature; is the atomic volume, *Z is thevalence of a migrating ion, and qe is the electron charge (the product
*
qZ e is
called the effective charge); U and l are the electric potential and the
characteristic length along the electric field; is the surface tension; x -
effective (far-field) external stress in the x-direction; is porosity.
E. Olevsky and L. Froyen, Constitutive modeling of spark-plasma sintering of conductive materials, Scripta Mater. 55, 1175-1178 (2006)
shrinkage due to grain-boundary diffusion
shrinkage due to dislocation creep
Constitutive Model of Spark-Plasma Sintering
C t ib ti f diff t f t t h i k d SPS
-
7/27/2019 0305 Olevsky - Theory of Sintering
54/64
Densification map for aluminum powder,T=673K, =28.3MPa
Contribution of different factors to shrinkage under SPS
E. Olevsky and L. Froyen, Constitutive modeling of spark-
plasma sintering of conductive materials, Scripta
Mater. 55, 1175-1178 (2006)
1.E-10
1.E-07
1.E-04
1.E-01
1.E+02
1.E+05
1.E+08
0.00 0.10 0.20 0.30 0.40 0.50 0.60
Porosity
ShrinkageR
ate,1/s
shrinkage rate due to electromigration (electric current)
shrinkage rate due to sintering stress (surface tension)
shrinkage rate due to power-law creep (punch load)
1.E-10
1.E-07
1.E-04
1.E-01
1.E+02
1.E+05
1.E+08
0.00 0.10 0.20 0.30 0.40 0.50 0.60
Porosity
ShrinkageR
ate,1/s
shrinkage rate due to electromigration (electric current)
shrinkage rate due to sintering stress (surface tension)
shrinkage rate due to power-law creep (punch load)
1.E-10
1.E-07
1.E-04
1.E-01
1.E+02
1.E+05
1.E+08
0.00 0.10 0.20 0.30 0.40 0.50 0.60
Porosity
ShrinkageR
ate,1/s
shrinkage rate due to electromigration (electric current)
shrinkage rate due to sintering stress (surface tension)
shrinkage rate due to power-law creep (punch load)
Grain Size: 1Grain Size: 40Grain Size: 100nm
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
1.E-08 1.E-07 1.E-06 1.E-05 1.E-04
Grain Size, m
Porosity
external load
surface tension
electromigration
Contribution of different factors to shrinkage rate of aluminum powder under SPS
417U Vl m
, T=6730K, x =28.3MPa
Shrinkage kinetics during SPS of aluminum powder:
-
7/27/2019 0305 Olevsky - Theory of Sintering
55/64
The average particle size is 55m. The applied field is accepted to be of
500V
m(Joule heat generation balancebased estimation), the pressure is
constant and equal to 23.5 MPa.
Shrinkage kinetics during SPS of aluminum powder:
comparison with experiments
Pressure 10 MPa
Field 250 V/m
10 MPa
250 V/m
E. Olevsky and L. Froyen, Constitutive modeling of spark-plasma sintering of conductive materials, Scripta Mater. 55, 1175-1178 (2006)
SUMMARY
-
7/27/2019 0305 Olevsky - Theory of Sintering
56/64
1. Science of Sintering: Fundamentals and
Historical Development2. Classical Models of Sintering: Viscous and
Diffusion Mechanisms of Mass Transport
3. Continuum Modeling of Powder Consolidation
4. Multi-Scale Modeling of Sintering5. Extrapolation of Sintering Concepts Towards
Constitutive Modeling of SPS
6. Sample SPS Problem Solutions
7. Further prospects of sintering modeling
SUMMARY
-
7/27/2019 0305 Olevsky - Theory of Sintering
57/64
(elV) 0
CpT
t
(kT T) el V2
ij (W)
Wij
.
1
3
e
.
ij
PLij
.
1 e
.
Conductive DC
Heat Transfer
by Conduction
Stress-Strain
Analysis
Densification
Coupled electro-thermo-mechanical FEM calculations
TEMPERATURE DISTRIBUTION DURING SPS
-
7/27/2019 0305 Olevsky - Theory of Sintering
58/64
prismatic die
temperature temperature gradient
temperature temperature gradient
cylindrical die
TEMPERATURE DISTRIBUTION DURING SPS
SPS SCALABILITY (SIZE DEPENDENCE)
-
7/27/2019 0305 Olevsky - Theory of Sintering
59/64
( )
Size 1 Size 2 Size 3 Size 4
SampleHeight[mm] 4 8 12 16Radius[mm] 7.5 15 22.5 30
DieHeight[mm] 30 60 90 120Radius[mm] 15 30 45 60
PunchHeight[mm] 20 40 60 80
RamHeight[mm] 40 80 120 160Radius[mm] 40 80 120 160
Alumina Disk-Shape Specimens (Same Aspect Ratio):
experimental verification
(size 2):
temperature evolution porosity evolution
SPS SCALABILITY (SIZE DEPENDENCE)
-
7/27/2019 0305 Olevsky - Theory of Sintering
60/64
SPS SCALABILITY (SIZE DEPENDENCE)
SPS SCALABILITY (SIZE DEPENDENCE)
-
7/27/2019 0305 Olevsky - Theory of Sintering
61/64
SPS SCALABILITY (SIZE DEPENDENCE)
-1.00
-0.80
-0.60
-0.40
-0.20
0.00
0.20
0.40
0.015 0.030 0.045 0.060
(Porosity(Cent
er)
Porosity(Surface))/SampleRadius
Die Radius [m]
Porosity Gradient
0.219
0.106
0.216
0.187
0.195
0.153
0.175
0.140
SPS SCALABILITY (SIZE DEPENDENCE): GRAIN GROWTH
-
7/27/2019 0305 Olevsky - Theory of Sintering
62/64
SPS Setup Geometry
Grain Size Evolution at Sample Center Grain Size Evolution at Sample Surface
Plane used for
displaying results
Die
Ram
Punch
Ram
Grain Size Gradient
0.0E+00
5.0E-09
1.0E-08
1.5E-08
2.0E-08
2.5E-08
3.0E-08
3.5E-08
0.015 0.030 0.045 0.060
(GrainSize(Cente
r)
GrainSize
(Surface))/Sam
pleRadius
Die Radius [m]
SUMMARY
-
7/27/2019 0305 Olevsky - Theory of Sintering
63/64
1. Science of Sintering: Fundamentals and
Historical Development2. Classical Models of Sintering: Viscous and
Diffusion Mechanisms of Mass Transport
3. Continuum Modeling of Powder Consolidation
4. Multi-Scale Modeling of Sintering5. Extrapolation of Sintering Concepts Towards
Constitutive Modeling of SPS
6. Sample SPS Problem Solutions
7. Further prospects of sintering modeling
SUMMARY
F rther prospects
-
7/27/2019 0305 Olevsky - Theory of Sintering
64/64
Development of on-line sintering damagecriteria
Modeling of nano-powder sintering
Modeling of sintering with phase
transformations or chemical reactionsModeling of field-assisted sintering
Development of sintering optimization
approaches
Multi-scale modeling of sintering
Further prospects