2.76/2.760 Multiscale Systems Design & Manufacturing
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1 2.76/2.760 Multiscale Systems Design & Manufacturing Fall 2004 Polymer, Protein, Complexity
2 Nanoimprinting PMMA silicon Dry etching Heat & Pressure Metal Lift-off Cooling & Separation Remove polymer S. Chou, Princeton
3 Nanoimprinting Photos removed for copyright reasons. Soft Lithography: PDMS
4 Nanopatterning by Diblock Copolymer Diagrams and photos removed for copyright reasons. See Park, M. et al. Science, Vol 276, 140, 1997
5 Di-block copolymers Gm = H 2 G < 0 X 2 m T S m composition Spinodal decomposition Free energy, G Spatial coordinate s 1 s 2 X 1 X 2 2 G X 2 = 0 composition
6 Di-block copolymer, PS-PMMA: PS+PMMA copolymers Diagrams removed for copyright reasons. PMMA <10% PMMA <30% PMMA 50%
7 Polymers, Macromolecules Poly (many) + mer (structural unit) -[C 2 H 4 ] n -,poly[ethylene] spaghetti H H H H C C C C H H H H
8 Configurational Entropy high entropy low
9 A singly bonded carbon chain N-2 angles g + ϕ θ, ϕ C n g C n-1 θ C n-2 θ=68 C n-3
10 Diffusion Brownian motion Albert Einstein: Worked out a quantitative description of Brownian motion based on the Molecular-Kinetic Theory of Heat (Nobel Prize 1921) R = 6Dt
11 Random Walk-1D -n n A simple coin toss Head +1 step Tail -1 step After n steps, where you will be located? o Gaussian lim n n λ k = 0 k=0 RMS= nλ frequency -Na 0 Na
12 Random walk -2D A drunkard nλ
13 Entropic Behaviour Size & Shape of Polymer Configurational Entropy Paul Flory (Stanford): Nobel Prize 1974 Pierre-Gilles de Gennes (Paris): Nobel Prize (1991) Stretched n a a Coiled End to end distance= a n
14 Possible Configurations P(r) P r 1 2na ( ) r = n e 2 2 P(r); the number of possible configurations of a random polymer coil with n segments of size a with an end-to-end distance (stretch) of r 0 R = a 0 n na
15 Entropy Stretching the coil Compressing the coil 2 3 r S = [ R 0 R r ] Random walk of unit polymer chain of 5 Angstroms Length=5 micron Ro=5 angstroms x 100=50 nm Volume at the highest entropy Real volume is twice bigger than that of RWM.
16 Self Avoiding Walk Polymers cannot cross its own path. Stotal = Spressure + Sdeformation RW SAW r R0 S = a n r [ + ] R0 r R 0 = an For maximum entropy 0.6
17 Nano-scale Phase Separation Random walk, Gaussian distribution e-to-e distance, R = an 1/2 R g = an 1/2 /6 N: number of monomers Micro-domain periodicity, L L R g an 1 2 N=1,000 a=5 angstroms Then, L is around 15 nm.
18 Polymers Synthetic versus Biological Synthetic Polymer Mostly chain like structure of repeated units (mers) Molecular weight distribution (chemical synthesis) Self avoiding walk model Protein Primary structure exactly defined Fixed molecular weight Unique folding Diagram removed for copyright reasons.
19 Proteins Proteins are polymers composed of amino acid monomers Proteins are characterized by a specific primary structure order of mers in the backbone and DP Control of primary structure leads to control of 3D structure Secondary structure refers to local chain conformations four types are known: α helix regular helix β sheet extended zig-zag β turn puts fold into β sheet Globular or random coil Tertiary structure refers to secondary structure stabilized by H bonds defines protein folding The control of protein structure builds information into the molecule that translates into function
20 Folding Summary Figure by OCW. (a) Linear Sequence of peptides. (b) Local folding into specific peptide backbone conformations. (c) Folded 3-dimensional structure of a single polypeptide chain. (d) Specific aggregation of two or more, identical or not, polypeptide chains.
21 Common 2ndary Structures α helix β sheet Collagen triple helix Globular or random coil Diagrams removed for copyright reasons.
22 Polymers vs. Protein Structure formation in synthetic polymers is statistically driven. Structure is metastable Interpenetration Structure formation in proteins is site specific chemistry driven. Structure is stable No interpenetration Misfolded proteins lead to serious diseases.
23 What is Complexity? natural DNA ~2-1/2 nm diameter Human heart Design for Manufacturing? Stata Center by Gehry $300 million, 5years Diagrams removed for copyright reasons. Human body (circulatory system) manmade Carbon nanotube ~2 nm diameter Simmons Hall $ 90million, 2 years Nanotube transistor
24 Scale Orders Scale order, N = size of the system smallest characteristic length Cars: 5 m 500 µ Jig Machines: 5 m 5 µ Lithography M/C: 30 cm 30 nm Human Body: 2 m 2 nm N Length scale of the periodicity?
25 Micro-phase Separation Random walk, Gaussian distribution e-to-e distance, R = an 1/2 R g = an 1/2 /6 N: number of monomers Micro-domain periodicity, L L R g an 1 2 N=1,000 a=5 angstroms Then, L is around 15 nm.
26 Complex Problems Gaussian integrals like Stock market index one year from today Weather one year from today
27 Complexity Universe Real Complexity (Uncertainty) (Complexity) Combinatorial Complexity (highly coupled, high scale order) Imaginary (decoupled, path dependent) (Difficulty) Periodic (uncoupled, smaller order)
28 What to How Good Design Top to Bottom What How Axiomatic approach - Does scale matter? How Independence Axiom Information Axiom Design Prof. Nam Parameters Evolution to Complexity Theory for Nano Systems
29 Information Axiom Minimize the Information Content 1 I = log2 = log2p P P : Probability of success =common range/system range Probability density bias Design range System range Common range FR
30 Complexity Time Dependent Combinatorial Complexity Time Independent Real Uncertainty Complexity Time Dependent Periodic Difficulty Time Independent Imaginary
31 Causality of Complexity Type III: difficulty Type I: coupling C Imaginary complexity Combinatorial complexity A D Large scale order complexity Type IV: non-equilibrium E Small scale order complexity Real Complexity B Type II: uncertainty
32 Complexity A system is complex when; A design is coupled. System ranges vary with time. The outcome is uncertain. (low probability of success) The scale order is very high. (over 10 9 ) Complexity can be reduced by; Periodic functions (temporal, spatial, etc.) Sang-Gook Kim
33 Functional Periodicity Time indepenedent real and imaginary complecity. Time dependent combinatorial and periodic complexity. Time dependent combinatorial complexity can become periodic complexity by functional periodicity. [Suh, ] Temporal Geometrical Biological Manufacturing process Chemical information Circadian etc. Sang-Gook Kim
34 Multi-scale system assembly by periodic building blocks? Periodic microdomains Functionally uncoupled domains Periodicity, Nano to Macro Biomimetic? Tendon hierarchy Simmons Hall Figure by OCW. L R g an 1 2
35 Block Assembly Nanopelleting Technique Silicon trenches DBCP pellets on Silicon Detachment (lift-off) Self-assembly
36 Bundle CNT nanopellet CMPed and Transplanted Photos removed for copyright reasons. See T. El-Aguizy, J-h Jeong, Y. B. Jeon, W. Z. Li, Z. F. Ren and S.G. Kim, "Transplanting Carbon Nanotubes", Applied Physics Letters, Vol 85, No. 25, P.5995, 2004
37 High aspect ratio nanopellets Cold cathode array, FED, Data storage, Multi-E-beam array for NGL Nanocandles 1-2 microns bundle Single strand
38 In-Plane Assembly of High-Aspect Ratio Nanocandle Mechanical in-plane assembly of nanocandle in the V-groove with a micro probe tip Bonding of nanocandle in the V-groove with a drop of epoxy Micro probe tip SU-8 CNT Nanocandle SEM of the assembly
39 Nanopipette Nanotube assembly to the tip of a micropipette SCNT Nanopellet micropipette Nanotube assembly to the tip of an in-plane AFM - Parallel Imaging and Pipetting - Multi-energy probing - Manufacturable - Arrayable
40 A multiscale system design Customer s needs Functionalities Design parameters Process variables m Nano-enabled products + µm Functionality Microstructures + Manufacturability Nano-structures nm Complexity NanoManufacturing
AXIOMATIC DESIGN OF MULTI-SCALE SYSTEMS
Proceedings of ICAD2004 ICAD-2004-29 Sang-Gook Kim sangkim@mit.edu Micro And Nano Systems Laboratory, Department of Mechanical Engineering Massachusetts Institute of Technology, Cambridge, MA 02139, USA
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