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EXTREME ENVIRONMENTS:o temperatureso ion concentrationso humiditieso stresseso transport rateso radiation fields
APPLICATIONS:o energy storage & conversiono environmental sensorso nuclear fuel & infrastructureo corrosion preventiono space & deep sea scienceo cancer microenvironments
MASSACHUSETTS INSTITUTE OF TECHNOLOGY
Krystyn J. Van VlietDepartments of Materials Science & Engineering and Biological Engineering
MIT, Cambridge, MA 02139AFOSR PECASE: Reactive Nanocomposites for Tunable Energy Dissipation
AFOSR Workshop on Materials & Processes Far From EquilibriumNov. 3-4, 2010
EXTREME ENVIRONMENTS:o temperatureso ion concentrationso humiditieso stresseso transport rateso radiation fields
APPLICATIONS:o energy storage & conversiono environmental sensorso nuclear fuel & infrastructureo corrosion preventiono space & deep sea scienceo cancer microenvironments
The MIT Center for Scientific Investigation of Materials in Extreme Environments aims to:• Connect researchers working in this diverse application space• Identify experimental & computational synergies and needs• Create new research & funding opportunities for students and faculty• Communicate CeSIMEE strengths to MIT, industry, and government
CeSIMEE Fall Lunch Forums: October 25 * November 15 * December 6
Massachusetts Institute of Technology
• Plasma Surface Interaction Science Center• Fusion energy & plasma thrusters• Whyte et al. (NSE)
• DOE Chemomechanics of Far-From-Equilibrium Interfaces (COFFEI)• Battery and solid-oxide-fuel cell materials at high flux and temperature• Tuller, Chiang, Carter, Van Vliet (MSE); Shao-Horn (ME); Yildiz, Yip (NSE)
• BP-MIT-Manchester Corrosion Center• Metal oxidation & corrosion at high acidity and temperature• Thomas, Schuh, Demkovicz, Gradecak (MSE); Yip, Yildiz (NSE)
• MIT Concrete Sustainability Hub• Predictive design of cement under extreme physical & mechanical environments• Jennings, Ulm, Pellenq (CEE); Van Vliet, Grossman, Yip, Marzari (MSE) et al.
• DOE Energy Hub – Consortium for Advanced Simulation of Light Water Reactors• Design of materials for nuclear reactor fuel and fuel cladding• Kazimi, Yip, Buongiorno, Yildiz (NSE); Demkovicz, Grossman (MSE) et al.
• Institute for Soldier Nanotechnology• Materials for blast & ballistic protection, tissue surrogacy• Radovitzky (AAE), Boyce, Socrate (ME), Thomas, Van Vliet (MSE)
• Biological/Biomedical Centers-To-Be…• Cancer & wound healing; deep-sea & acidophilic organisms; space travel; NMR imaging• Van Vliet, Ortiz, Gibson (MSE); Newman (AAE); Jasanoff, Alm (BE); others?
Connecting interdisciplinary materials research10
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11.1
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http://cesimee.mit.edu * Supported jointly by MIT Department of Materials Science & Engineering and MIT Nuclear Science & Engineering
• Plasma Surface Interaction Science Center• Fusion energy & plasma thrusters• Whyte et al. (NSE)
• DOE Chemomechanics of Far-From-Equilibrium Interfaces (COFFEI)• Battery and solid-oxide-fuel cell materials at high flux and temperature• Tuller, Chiang, Carter, Van Vliet (MSE); Shao-Horn (ME); Yildiz, Yip (NSE)
• BP-MIT-Manchester Corrosion Center• Metal oxidation & corrosion at high acidity and temperature• Thomas, Schuh, Demkovicz, Gradecak (MSE); Yip, Yildiz (NSE)
• MIT Concrete Sustainability Hub• Predictive design of cement under extreme physical & mechanical environments• Jennings, Ulm, Pellenq (CEE); Van Vliet, Grossman, Yip, Marzari (MSE) et al.
• DOE Energy Hub – Consortium for Advanced Simulation of Light Water Reactors• Design of materials for nuclear reactor fuel and fuel cladding• Kazimi, Yip, Buongiorno, Yildiz (NSE); Demkovicz, Grossman (MSE) et al.
• Institute for Soldier Nanotechnology• Materials for blast & ballistic protection, tissue surrogacy• Radovitzky (AAE), Boyce, Socrate (ME), Thomas, Van Vliet (MSE)
• Biological/Biomedical Centers-To-Be…• Cancer & wound healing; deep-sea & acidophilic organisms; space travel; NMR imaging• Van Vliet, Ortiz, Gibson (MSE); Newman (AAE); Jasanoff, Alm (BE); others?
Connecting interdisciplinary materials research
http://cesimee.mit.edu * Supported jointly by MIT Department of Materials Science & Engineering and MIT Nuclear Science & Engineering
COFFEI: Chemomechanics of Far-From-Equilibrium InterfacesW. Craig Carter, Yet-Ming Chiang, Yang Shao-Horn, Krystyn Van Vliet, Bilge Yildiz, Sidney Yip, Harry Tuller (PI)
Project Goal: To develop understanding of the electro-chemo-mechanical coupling of defect concentrations, ionic transport, and stored elastic energy in far-from-equilibrium conditions typical of energy device applications
• Thermal expansion and mismatch:
• Thermal Shock:
We wouldn’t think of putting materials in service without considering their thermal-mechanical properties
€
εthermal = α LΔT
schenectady.k12.ny.us
frca.co.uk
Thermomechanical vs. Chemomechanical Properties
http://en.wikipedia.org/wiki/Liberty_Bell
€
RT =kσT (1 −ν )
αEk = thermal⋅ conductivity
σT = max imum⋅ tension
α = thermal⋅ exp ansion⋅ coeff .
E = Young 's⋅mod ulus
υ = Poisson⋅ ratio
think-aboutit.com
H2
O2
DLi
DO
Fresh Cell
50 Cycles
Ion transport in battery & fuel cell nano-oxides:“Electrochemical shock”
Critical combinati
ons of particle size and
rate
Now validated via our
nanoparticle & nanofilm fracture
toughness measurements
J. Electrochem. Soc., 157 [10] A1052-A1059 (2010)
New Electromechanical Shock Maps
Unique experimental tools in FFE environments
f → mass
O2 (g)Vibrating substrate
V
L/L
Load
Thin film
Substrate
Nanoindentation at high temps (1000C) and controlled
gas environments
Scanning Tunneling Microscopy & XPS:Electrochemistry in situ
Krystyn J. Van Vliet, Roland Pellenq, Jeff Grossman, Bilge Yildiz, Sid Yip, Franz Ulm
web.mit.edu/cshub
MIT Concrete Sustainability Hub:Redesign from first principles
MotivationUnderstanding dehydration effects in cement & concrete is:• Key to minimizing shrinkage and cracking in slabs & pavements• Key to Air Force runway durability & repair
0.0 0.2 0.4 0.6 0.8 1.0
0
5
10
15
20
25
Water Content ( mass % )
p/ps
Powers and Brownyard (1946)
Wat
er C
onte
nt [%
mas
s]
Partial Pressure [p/ps]
Water adsorption dynamics poorly understood, widely studied
http://www.cement.org
Temperature, humidity, & drying Shrinkage, cracking, warping, reduced lifespan
Can molecular modeling shrink this problem?
Unique FFE computational tools: atomistic modeling• How many H2O molecules occupy C-S-H atomistic model at
specific humidity, temperature, or pressure?
C-S-H (, V, T)
equilibrium
H2O (, V, T)
non-equilibrium
-0.2 0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.81
2
3
4
5
6
7
8
Hardness (GPa)
Mole ratio of H2O/Si
Cement mechanical strength scales with H2O content
• Up to 30 vol% shrinkage as C-S-H fully dehydrated• Shear strength doubles as C-S-H density decreases
-0.05 0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
full dry
Pxz (GPa)
strain = angle change in radian
XZ shear
τmax
τmax
shear strain
she
ar
stre
ss [
GP
a]
max3 τ×=Hardness
tmax
fully hydrated C-S-H
fully dry C-S-H
H2O/Si [mol/mol]
Plasma Surface Interaction Science CenterDennis Whyte et al.
• ITER Mission: – Exothermic “Burn” Q=10
• Reactor level fusion power– Pfusion ~ 400 MW for 500 s– Heating = 40 MW– 20% duty cycle
• Size R~6 m +Field B~6 T = 5 Billion dollars– 1000 m3 plasma– 1000 m2 plasma-facing wall
The Multi-Scale, Synergistic Plasma-Surface Interface
No materials currently exist to withstand high dpa, high temps, and plasma erosion resistance required
Issue / ParameterPresent
Tokamaks ITER DEMO Consequences
Quiescent energy exhaustGJ / day ~ 10 3,000 60,000
- active cooling- max. tile thickness ~ 10 mm
Transient energy exhaust from plasma instabilities T~ MJ / Awall(m2) / (1 ms)1/2
~ 2 15 60
- require high Tmelt/ablate
- limit? ~ 60 for C and W - surface distortion
Yearly neutron damage in plasma-facing materialsdisplacements per atom
~ 0 ~ 0.5 20
- evolving material properties: thermal conductivity & swelling
Max. gross material removal rate with 1% erosion yield(mm / operational-year)
< 1 300 3000
- must redeposit locally- limits lifetime- produces films
Tritium consumption(g / day) < 0.02 20 1000
- Tritium retention in materials and recovery
Unique FFE experimental tools:MIT CLASS/DIONISOS facility has unique dynamic PSI capabilities:
Real-time, non-perturbing MeV ion-beam surface analysis simultaneous with cw, high intensity plasma exposure
• Real-time, depth-resolved, spatially dependent measurements of• Erosion• Film growth• Element/isotope mix• Fuel storage (H, He, Ar)
PSI Science Center, leveraging world-class US university PSI capabilities
UC Berkeley / Tennessee Materials Modeling(Wirth)
MIT / DIONISOS(Director: Whyte)
UCSD / PISCES (Doerner)
Emphasizing multidisciplinary training of young scientists & strong, multi-institutional collaborations
• Plasma Surface Interaction Science Center• Fusion energy & plasma thrusters• Whyte et al. (NSE)
• DOE Chemomechanics of Far-From-Equilibrium Interfaces (COFFEI)• Battery and solid-oxide-fuel cell materials at high flux and temperature• Tuller, Chiang, Carter, Van Vliet (MSE); Shao-Horn (ME); Yildiz, Yip (NSE)
• BP-MIT-Manchester Corrosion Center• Metal oxidation & corrosion at high acidity and temperature• Thomas, Schuh, Demkovicz, Gradecak (MSE); Yip, Yildiz (NSE)
• MIT Concrete Sustainability Hub• Predictive design of cement under extreme physical & mechanical environments• Jennings, Ulm, Pellenq (CEE); Van Vliet, Grossman, Yip, Marzari (MSE) et al.
• DOE Energy Hub – Consortium for Advanced Simulation of Light Water Reactors• Design of materials for nuclear reactor fuel and fuel cladding• Kazimi, Yip, Buongiorno, Yildiz (NSE); Demkovicz, Grossman (MSE) et al.
• Institute for Soldier Nanotechnology• Materials for blast & ballistic protection, tissue surrogacy• Radovitzky (AAE), Boyce, Socrate (ME), Thomas, Van Vliet (MSE)
• Biological/Biomedical Centers-To-Be…• Cancer & wound healing; deep-sea & acidophilic organisms; space travel; NMR imaging• Van Vliet, Ortiz, Gibson (MSE); Newman (AAE); Jasanoff, Alm (BE); others?
Connecting interdisciplinary materials research
http://cesimee.mit.edu * Supported jointly by MIT Department of Materials Science & Engineering and MIT Nuclear Science & Engineering