Title: High-Efficiency, Scalable Solar Cells of Earth-Abundant Materials
13.40/22.71
- Summary of 10/23/2012
- Sergio Castellanos
- Mechanical Engineering Department
- Massachusetts Institute of Technology, Cambridge,
MA (USA)
2Stress-Strain
s
- Constitutive Relations
- Strength A
- Ductility B
- Toughness C
e
3Inelastic Processes
- Plasticity
- Phase Transformation
Potential Energy (V)
Potential Energy (V)
Non-Periodic
Periodic
Cleavage Opening
Slip Displacement
V0
Total Metal-Metal Coordination remains constant
One-off dissipation mechanism
4Inelastic Processes in Metals
- Easier to follow the path of plasticity
(sustainable dissipation) - Fracture toughness Resistance against crack
propagation
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
Metallic Ionic Covalent
S. Ogata and J. Li Toughness scale from first
principles J. Appl. Phys. 106, 113534 (2009)
5Inelastic Processes in Metals
- Easier to follow the path of plasticity
(sustainable dissipation) - Fracture toughness Resistance against crack
propagation
BBulk Modulus GShear Modulus OCell Volume
- KIC function of
- Bonding energy
- Ideal strength
- Bandgap
- Ionicity
S. Ogata and J. Li Toughness scale from first
principles J. Appl. Phys. 106, (2009) 113534
6Flow in the presence of Diffusion Creep
Input
Output
s
e
e(t-to)
so
eo
to
t
t
to
- Different stages on Creep
- Progression towards steady state flow (s.s.
dislocation density gen.) - Static recovery counterbalances new dislocation
generation - Terminal failure (e.g. necking in tension test)
7Deformation-Mechanism Map
Frost, Harold Jefferson, and M. F. Ashby.
"Deformation-mechanism maps The plasticity and
creep of metals and ceramics. Pergamon Press,
Oxford, UK (1982).
8Deformation-Mechanism Map
Limit on Ideal Shear Strength
Low T plasticity by dislocation glide and
twinning Limited by Discrete
obstacles Lattice Friction
Displacive
Power Law by Glide / Glide Climb Limited
by Glide processes Lattice-Diffusion
controlled climb Core-Diffusion controlled
climb Breakdown Harper-Dorn Dynamic
Recristallization
Mixed
Diffusional
Diffusional Flow Limited by Lattice-Diffusion
(Nabarro-Herring) GB Diffusion
(Coble) Interface-reaction controlled
Frost, Harold Jefferson, and M. F. Ashby.
"Deformation-mechanism maps The plasticity and
creep of metals and ceramics. Pergamon Press,
Oxford, UK (1982).
9Coble (Surface)
Nabarro-Herring (Lattice)
, Low T
, High T
DsurfacegtgtDbulk
Dsurface comparable Dbulk
1 Image from http//en.wikipedia.org/wiki/Frank_
Nabarro 2 Image from http//news.stanford.edu/ne
ws/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)
10Hall-Petch Smaller is Stronger
Copper
M.A. Meyers et al. Mechanical Properties of
nanocrystalline materials Progress in Materials
Science 51 (2006), 427-556
11Surface Dislocation Nucleation
- Nucleation Stress value computed
- Transition predicted from collective dislocation
dynamics to signle dislocation nucleation - Geomtry Long Range Elastic Interaction
(Corner/Image)
T. Zhu et al. Temperature and Strain-Rate
Dependence of Surface Dislocation Nucleation PRL
100, (2008) 025502
12Ultra-Strength Materials
- This implies that properties (thermal
conductivity, transmittance, etc) can be modified
while in the elastic regime.
DoE (Taguchi)
2
13Elastic-Strain Engineering
E
M G K M
Synthesize
Strain and Measure Force
Measure Strain
Numerical Prediction
- Graphene
- Carbon Nanotubes
- Bulk Nanocrystals
14Cool (or Hot?) Application Photovoltaics
1
Challenges - Thermalization Losses -
Non-Absorption Losses
2
1 Image http//en.wikibooks.org/wiki/Microtechn
ology/Semiconductors 2 Ji Feng et al.
Strain-Engineered Artificial Atom as a
Broad-Spectrum Solar Energy Funnel Nature (2012)
Accepted