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These slides have a special sentimental value to me: It presents a joint work with Olivier Coussy, one of my dearest friends.
Olivier Coussy
Achievements • Plenary lecture, Geoproc 2008 • Invited scientist, Princeton University, July 2007 • Keynote Lecture, Thermo-mechanical modelling for solids, Ecole polytechnique, 2007 • Invited Professor, Universitat Polytècnica de Cataluyna, May 2007 • Professor, Ecole des Ponts, in charge of the Lafarge research and master program, 2006 • Senior scientist of outstanding rank, 2006 • Berkeley-France funds award, 2005 • Visiting Research Scholar, University of Princeton, Spring semester 2005 • Visiting Miller Research Professor, University of California Berkeley, Fall semester 2004 • Plenary Lecture, Congrès Français de Thermique, 2004 • Biot Medal lecture, 2003, 16th ASCE Engineering Mechanics Conference, Seattle, 2003 • ASCE Biot Medal Award, 2003 • T.C. Powers Lecture, Concreep VI, 2001 • Knight of the National Order of Merit, 2000 • Plumey Award, 1999 (Award from the French Academy of Sciences in the field of
Mechanical Sciences) • Associate Professor, 1985-1997, Ecole Polytechnique • MTS Visiting professor, University of Minnesota, Spring semester 1995 • Associate Professor, 1992-1998, Université de Marne-la-Vallée • Plenary Lecture, Symposium Rock at Great Depths, 1989 • Jean Mandel Award, 1985
Our joint papers • P.J.M. Monteiro, Olivier Coussy, Denise A. Silva, Effect of cryo-suction
and air void transition layer on the hydraulic pressure developed during freezing of concrete, ACI Materials Journal, V. 103, No.2, 136-140, 2006.
• Olivier Coussy_and Paulo J.M. Monteiro, Unsaturated poroelasticity for crystallization in pores, Computers and Geotechnics 34 (2007) 279–290.
• O. Coussy_and P. J.M. Monteiro, Poroelastic model for concrete exposed to freezing temperatures, Cement and Concrete Research, Volume: 38, 40-48, 2008.
• A. Fabbri, O. Coussy, T. Fen-Chong and P.J.M. Monteiro, Are Deicing Salts Necessary to Promote Scaling in Concrete? Journal of Engineering Mechanics – ASCE, Volume: 134 Issue: 7 Pages: 589-598, JUL 2008.
• O. Coussy and P.J.M. Monteiro, Errata to “Poroelastic model for concrete exposed to freezing temperatures”[Cement and Concrete Research 38 (2008) 40–48], Cement and Concrete Research 39 (2009) 371–372.
If you’re interested in poromechanics
NAVIER INSTITUTE
Institut Navier Olivier Coussy
Unsaturated poroelasticity of freezing water-infiltrated materials with air voids
Miller Institute for Basic Research in Science, UC Berkeley
Paulo Monteiro Berkeley University
3 rd Biot Conference on Poromechanics, May 24-27 2005, Norman, Oklahoma
Bulk damage induced by frost action on a limestone
Outlines
1. Unsaturated poromechanics 2. Liquid saturation curve and
interfacial energy 3. Hydraulic pressure
4. Cryosuction 5. Air voids
Beaudoin, Mc Innis, 1974
motivations
unsaturated poromechanics liquid saturation curve hydraulic pressure cryosuction air voids
definitions
Solid matrix
unsaturated porous material
(as a whole)
interfaces
crystal
liquid
interfaces
+ =
porous solid =
solid matrix +
porous volume
bulk crystal and liquid
constituents
+
Skeleton Scale at which porosity, saturation degree, pore radius distribution are
relevant
unsaturated poromechanics liquid saturation curve hydraulic pressure cryosuction air voids
ρ φC C
ρ φL L
i jσ
i jε
0σ ε φ φ+ + − =i j i j C C L L skd p d p d dF
partial porosity
Skeleton
( ) ( ), , ,sk ij C L LF W U Sε ϕ ϕ φ φ= +
Interfacial energy Porous solid elastic free energy
Skeleton energy including the
interfacial energy
2 2 03 3
σ ε ϕ ϕ⎛ ⎞ ⎛ ⎞+ − + − − =⎜ ⎟ ⎜ ⎟⎝ ⎠ ⎝ ⎠
ij ij C C L Ld p U d p U d dW ( )C LL
dUp pdS
− − = −
0C C CSφ φ ϕ= +
Crystal saturation degree
Change due to deformation
Porous solid constitutive equations
Upscaling methods: K, G, bJ, NIJ are known as functions of ks, gs, SL, φ0
2 2 03 3
σ ε ϕ ϕ⎛ ⎞ ⎛ ⎞+ − + − − =⎜ ⎟ ⎜ ⎟⎝ ⎠ ⎝ ⎠
ij ij C C L Ld p U d p U d dW
unsaturated poromechanics liquid saturation curve hydraulic pressure cryosuction air voids
Solid matrix elastic modulis
0
0
1/ 1/ 2 / 31/ 1/ 2 / 3
ij ijkl C L ij
C C C C CC CL C
L L L L CL LL L
b bS b N N p US b N N p U
σ ε
ϕ φ φ
ϕ φ φ
Λ − −⎛ ⎞ ⎛ ⎞⎛ ⎞⎜ ⎟ ⎜ ⎟⎜ ⎟= − = − −⎜ ⎟ ⎜ ⎟⎜ ⎟⎜ ⎟ ⎜ ⎟⎜ ⎟= − − −⎝ ⎠ ⎝ ⎠⎝ ⎠
metastable
unsaturated poromechanics liquid saturation curve hydraulic pressure cryosuction air voids
C LL
dUp pdS
− = −
( )− = Σ −C L f fp p T T
(Thomson-Gibbs)
( )L LS Tσ=
from the capillary curve or by direct experimentation
-45°C 0°C 100°C
fT state function
*
⎛ ⎞⎜ ⎟⎜ ⎟⎜ ⎟⎜ ⎟⎝ ⎠
−= f
L
T TS f
T
2γ γγ∗ ∗
∗
= =Σ Σ
CL CL
f LG f
NT RT
12C L
CL
p pRγ
−=
12G L
LG
p pRγ
−=
0
100
200
300
0 20 40 60 80 100 0
25
50
75
100
SL (%)
p G -
pL (
MPa
)
h r (%
)
⎛ ⎞⎜ ⎟⎜ ⎟⎜ ⎟⎝ ⎠
−= G L
Lp pS fN
Capillary curve
-5 -4 -3 -2 -1 0 1 2 3
0.5
1
1.5
2
2.5
0.9
0.8
0.5 0.7
0.6
0.9 0.8
0.5 0.4
0.6 0.7
R * dS L / dR
S L
−( T f −T ) / T* R / R *
( )1 11 1
1 / 1 1m m
m m
fL C L
T T RS S T TT R
σ− −
− −
∗∗
∗
⎡ ⎤ ⎡ ⎤−⎛ ⎞ ⎛ ⎞⎢ ⎥= − = = + = +⎢ ⎥⎜ ⎟ ⎜ ⎟⎢ ⎥ ⎝ ⎠⎢ ⎥⎝ ⎠ ⎣ ⎦⎣ ⎦
1 2 3 4 50
0.2
0.4
0.6
0.8
1
1.2
1.4
U/S
fT *
( T f −T ) / T*
0.9 0.8 0.5 0.7 0.6
Interfacial energy Liquid saturation curves and pore radius distributions
unsaturated poromechanics liquid saturation curve hydraulic pressure cryosuction air voids
*
*
164.26nm
T KR=
=
cement paste
CRYOSTAT
Data acquisition 4 cm
By direct measurement: capacitive test
0
0,2
0,4
0,6
0,8
1
1,2
1,4
-3 -2,5 -2 -1,5 -1 -0,5 0 0,5 1 1,5 2
E / C = 0,5. T *= 7° C et R *= 9,1 nm
E / C = 0,4. T *= 9° C et R *= 7,3 nm
-‐( T f -‐T ) / T * R / R *
R * X dS L / dRS L
propagation Scherer, 1993
fT
fThomogeneous nucleation
2 ?CLf
f
T T RRSγ
= −
1 fT T<
2 1T T<
2R
unsaturated poromechanics liquid saturation curve hydraulic pressure cryosuction air voids
1 fT T<2R
2 1T T<
2R
hydraulic pressure (undeformable, Powers, 1949-1953)
liquid
air void
ice
Lp Z
unsaturated poromechanics liquid saturation curve hydraulic pressure cryosuction air voids
Undeformable
0
01 CL
L
dTpdt
ρρ
⎛ ⎞∝ − ×⎜ ⎟⎝ ⎠
Deformable: ε ?Unsaturated
poromechanics
liquid
unsaturated poromechanics liquid saturation curve hydraulic pressure cryosuction air voids
( )− = Σ −C L f fp p T T
pore radius distribution and saturation cryo-swelling
0 0.4 0.8 1.2 1.6 20
0.1
0.2
0.3
( T f −T ) / T*
0.9
0.8
0.5 0.7 0.6 0.4
Sf
10 3
-5 -4 -3 -2 -1 0 1 2 3
0.5
1
1.5
2
2.5
0.9
0.8
0.5 0.7
0.6
0.9 0.8
0.5 0.4
0.6 0.7
R * dS L / dR
S L
−( T f −T ) / T* R / R *
ice
T
T
air void ( )0
= −Σ −
=
L f f
C
p T T
p
unsaturated poromechanics liquid saturation curve hydraulic pressure cryosuction air voids
( )− = Σ −C L f fp p T T
T stops
P. Monteiro
air void
( )0
= −Σ −
=
L f f
C
p T T
p
overall shrinkage
T stops
0.5 1 1.5 - 2
- 1
0
1
2
3
t / τ * = ( T f - T) / T *
O ×
10 3
m = 0.7 m = 0.5
All effects accounted for, including thermal deformation !
no air voids
0 1 2 3 R/R*
120oC h−×
13oC h−×
with air voids Equilibrium
Damage due to salt crystallization
( )− = Σ −C L f fp p T T0
lnυ
− =C LC
nRT xp px
supersaturation
Extension to salt crystallization?
From Rijniers et al.
Conclusions
1. unsaturated poromechanics can be uselful
2. Liquid saturation degree as a thermodynamic state function of the temperature
3. Theory and experiments include:
1. pore radius distribution 2. surface effects 3. hydraulic pressure 4. cryosuction 5. air voids
… presence of chemicals, deicer salt, salt crystallization
Acknowledgments
Miller Institute
A. Fabbri (PhD, UMLV) T. Fen-Chong (Institut Navier)
G. Scherer (Princeton)
Recommended