3.40/22.71 Summary of 10/23/2012 Sergio Castellanos Mechanical Engineering Department Massachusetts...

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3.40/22.71 Summary of 10/23/2012 Sergio Castellanos Mechanical Engineering Department Massachusetts Institute of Technology, Cambridge, MA (USA)

Transcript of 3.40/22.71 Summary of 10/23/2012 Sergio Castellanos Mechanical Engineering Department Massachusetts...

Page 1: 3.40/22.71 Summary of 10/23/2012 Sergio Castellanos Mechanical Engineering Department Massachusetts Institute of Technology, Cambridge, MA (USA)

3.40/22.71

Summary of 10/23/2012

Sergio Castellanos

Mechanical Engineering DepartmentMassachusetts Institute of Technology, Cambridge, MA (USA)

Page 2: 3.40/22.71 Summary of 10/23/2012 Sergio Castellanos Mechanical Engineering Department Massachusetts Institute of Technology, Cambridge, MA (USA)

Stress-Strain

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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.

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Inelastic Processes

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• 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

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Easier to follow the path of plasticity (sustainable dissipation) Fracture toughness: Resistance against crack propagation

Inelastic Processes in Metals

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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

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Easier to follow the path of plasticity (sustainable dissipation) Fracture toughness: Resistance against crack propagation

Inelastic Processes in Metals

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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

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Flow in the presence of Diffusion: Creep

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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)

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Deformation-Mechanism Map

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Frost, Harold Jefferson, and M. F. Ashby. "Deformation-mechanism maps: The plasticity and creep of metals and ceramics.” Pergamon Press, Oxford, UK (1982).

Page 8: 3.40/22.71 Summary of 10/23/2012 Sergio Castellanos Mechanical Engineering Department Massachusetts Institute of Technology, Cambridge, MA (USA)

Deformation-Mechanism Map

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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

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•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

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Hall-Petch: Smaller is Stronger

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Copper

M.A. Meyers et al. “Mechanical Properties of nanocrystalline materials” Progress in Materials Science 51 (2006), 427-556

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Nucleation Stress value computed

Transition predicted from collective dislocation dynamics to signle dislocation nucleation

Geomtry = Long Range Elastic Interaction (Corner/Image)

Surface Dislocation Nucleation

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T. Zhu et al. “Temperature and Strain-Rate Dependence of Surface Dislocation Nucleation” PRL 100, (2008) 025502

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Ultra-Strength Materials

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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

)

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Elastic-Strain Engineering

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Synthesize Strain and Measure Force

Measure Strain

E

M Γ K M

NumericalPrediction

• Graphene• Carbon Nanotubes• Bulk Nanocrystals

• AFM • Synchrotron• In-situ TEM

• DFT

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Cool (or Hot?) Application: Photovoltaics

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[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]