3.40/22.71 Summary of 10/23/2012 Sergio Castellanos Mechanical Engineering Department Massachusetts...
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Transcript of 3.40/22.71 Summary of 10/23/2012 Sergio Castellanos Mechanical Engineering Department Massachusetts...
3.40/22.71
Summary of 10/23/2012
Sergio Castellanos
Mechanical Engineering DepartmentMassachusetts Institute of Technology, Cambridge, MA (USA)
Stress-Strain
2
Constitutive Relations: Strength [A] Ductility [B] Toughness [C]
σ
ε
A
B
C
E [Pa]
εplastic εelastic ε
σ Upon unloading εtotal = εplastic + εelastic
I.e. Springback
Hysteresis Loop.- Dissipation converts useful mechanical energy into heat.
Inelastic Processes
3
• Plasticity• Phase
Transformation
• Plasticity• Phase
Transformation
• Fracture• Fracture
Pot
entia
lE
nerg
y (V
)
Slip DisplacementP
oten
tial
Ene
rgy
(V)
Cleavage Opening
Total Metal-Metal Coordination remains constant
One-off dissipation mechanism
V”=0
PeriodicNon-Periodic
Easier to follow the path of plasticity (sustainable dissipation) Fracture toughness: Resistance against crack propagation
Inelastic Processes in Metals
4
Material KIC-Max [MPa/m0.5]
Cu 107
Ag 105
Fe 150
Ni 150
W 150
SiC 5.1
B-Si3N4 10
TiC 3
MgO 2.8
NaCl 0.19
S. Ogata and J. Li “Toughness scale from first principles” J. Appl. Phys. 106, 113534 (2009)
MetallicIonicCovalent
Easier to follow the path of plasticity (sustainable dissipation) Fracture toughness: Resistance against crack propagation
Inelastic Processes in Metals
5
S. Ogata and J. Li “Toughness scale from first principles” J. Appl. Phys. 106, (2009) 113534
• KIC function of:- Bonding energy- Ideal strength- Bandgap- Ionicity
•
€
˜ K =K IC
B⋅Ω1
6 B=Bulk ModulusG=Shear ModulusΩ=Cell Volume
Shear Weak = Energy Dislocation Spread = KIC
Flow in the presence of Diffusion: Creep
6
σ
t t
ε
toto
Input
σo
εo
ε(t-to)
Output
Different stages on Creep:1. Progression towards steady state flow (s.s. dislocation density – gen.)2. Static recovery counterbalances new dislocation generation3. Terminal failure (e.g. necking in tension test)
…
Deformation-Mechanism Map
7
Frost, Harold Jefferson, and M. F. Ashby. "Deformation-mechanism maps: The plasticity and creep of metals and ceramics.” Pergamon Press, Oxford, UK (1982).
Deformation-Mechanism Map
8
Frost, Harold Jefferson, and M. F. Ashby. "Deformation-mechanism maps: The plasticity and creep of metals and ceramics.” Pergamon Press, Oxford, UK (1982).
Limit on Ideal Shear Strength
Low T plasticity by dislocation glideand twinning Limited by:
Discrete obstaclesLattice Friction
Power Law by Glide / Glide + ClimbLimited by:
Glide processesLattice-Diffusion controlled climbCore-Diffusion controlled climbBreakdownHarper-DornDynamic Recristallization
Diffusional FlowLimited by:
Lattice-Diffusion (Nabarro-Herring)GB Diffusion (Coble)Interface-reaction controlled
DisplaciveDisplacive
DiffusionalDiffusional
MixedMixed
9
•Does not involve dislocations.
• Through bulk or along free surfaces
•Does not involve dislocations.
• Through bulk or along free surfaces
Diffusional
[1] Image from http://en.wikipedia.org/wiki/Frank_Nabarro[2] Image from http://news.stanford.edu/news/2009/july27/herring-physics-obit-073109.html[3] Brown, L.M. “Frank Reginald Nunes Nabarro MBE” Biographical Memoirs of Fellows of the Royal Society (2009)
-
Nabarro-Herring(Lattice)
Coble(Surface)
, High T, Low T
Dsurface>>Dbulk Dsurface comparable Dbulk
Hall-Petch: Smaller is Stronger
10
Copper
M.A. Meyers et al. “Mechanical Properties of nanocrystalline materials” Progress in Materials Science 51 (2006), 427-556
Nucleation Stress value computed
Transition predicted from collective dislocation dynamics to signle dislocation nucleation
Geomtry = Long Range Elastic Interaction (Corner/Image)
Surface Dislocation Nucleation
11
T. Zhu et al. “Temperature and Strain-Rate Dependence of Surface Dislocation Nucleation” PRL 100, (2008) 025502
Ultra-Strength Materials
12
€
τcrit >τ shear _ ideal
10=
G
10
ε elastic >1
100=1%
This implies that properties (thermal conductivity, transmittance, etc) can be modified while in the elastic regime.
Hydrostatic: phase transformation
[1] Yanming Ma et al. “Transparent Dense Sodium” Nature 458, (2009) 182[2] Images from ti-fr.com, nutritionresearchcenter.org
[1]
€
d(Ppty) = ∂ε ⋅∂(Ppty)
∂ε> 0Elastic-Strain Engineering
[2]
DoE(Taguchi
)
DoE(Taguchi
)
Elastic-Strain Engineering
13
Synthesize Strain and Measure Force
Measure Strain
E
M Γ K M
NumericalPrediction
• Graphene• Carbon Nanotubes• Bulk Nanocrystals
• AFM • Synchrotron• In-situ TEM
• DFT
Cool (or Hot?) Application: Photovoltaics
14
[1] Image: http://en.wikibooks.org/wiki/Microtechnology/Semiconductors[2] Ji Feng et al. “Strain-Engineered Artificial Atom as a Broad-Spectrum Solar Energy Funnel” Nature (2012)
Accepted
Challenges:- Thermalization Losses - Non-Absorption Losses
[2]
[1]