NSF NIRT Grant 0609115 Hierarchical Nanomanufacturing of Carbon Nanotube Sheets and Yarns and their Applications for Active Nano-Materials Systems PIs:

Slides:



Advertisements
Similar presentations
Mechanical Properties of the NCSX Modular Coil Conductor 14 January 2004 Leonard Myatt Myatt Consulting, Inc.
Advertisements

Forms of Carbon. Diamond Covalent crystals: C, Si, Ge, SiC Strong sp 3  bonds form tetrahedral structure Face Centered Cubic lattice (fcc) –8 C atoms.
MECHANICAL PROPERTIES
Normal Strain and Stress
Distribution of Microcracks in Rocks Uniform As in igneous rocks where microcrack density is not related to local structures but rather to a pervasive.
Chun-Chieh Lu Carbon-based devices on flexible substrate 1.
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Interacting charge and spin chains in high magnetic fields James S. Brooks, Florida State University, DMR [1] D. Graf et al., High Magnetic Field.
DMR :Electronic Correlations in Carbon Nanotube Apparao M. Rao José Menéndez Damping of vibrations in carbon nanotubes Tunneling and optical experiments.
Metal-free-catalyst for the growth of Single Walled Carbon Nanotubes P. Ashburn, T. Uchino, C.H. de Groot School of Electronics and Computer Science D.C.
Yi Rao, UC Berkeley1 Carbon Nanotube (CNT) Aerogel Muscles Yi Rao May 4th, 2008.
CHAPTER OBJECTIVES Apply the stress transformation methods derived in Chapter 9 to similarly transform strain Discuss various ways of measuring strain.
CNT – Characteristics and Applications
Computational Materials Science Network Grain Boundary Migration Mechanism:  Tilt Boundaries Hao Zhang, David J. Srolovitz Princeton Institute for the.
Interconnect Focus Center e¯e¯ e¯e¯ e¯e¯ e¯e¯ SEMICONDUCTOR SUPPLIERS Goal: Fabricate and perform electrical tests on various interconnected networks of.
CM 197 Mechanics of Materials Chap 14: Stresses in Beams
Assist.Prof.Dr. Ahmet Erklig
Institute of Optics, University of Rochester1 Carbon Nanotubes: theory and applications Yijing Fu 1, Qing Yu 2 1 Institute of Optics, University of Rochester.
Nanoscale memory cell based on a nanoelectromechanical switched capacitor EECS Min Hee Cho.
Steve Cronin University of Southern California Electrical Engineering - Electrophysics Optical and Electronic Measurements of Individual Carbon Nanotubes.
FIBROUS REINFORCEMENT Structure: 1.Continuous bundles of fibers. 2.Woven fabrics. 3.Chopped fiber.
Gauss’ Law.
Periodic table. 2 3 Periodic trends in the properties of atoms One of the most fundamental principles of chemistry is the periodic law, states that,
Northwestern University Rod Ruoff Nanotechnology Fracture Mechanics of One- Dimensional Nanostructures.
Theoretical Analysis of a Nanosensor based on WO 3 coated Carbon Nanotube for Ultra-high Sensitive Breath Acetone Sensing Ming Xia, Advisor: Prof. Xingguo.
Self-assembled MoSIx Nanowire Networks Jure Strle adviser: prof. dr. Dragan Mihailovič February 2008 University of Ljubljana Faculty of mathematics and.
LOGO What a rule surfactants play in synthesis CNTs array Shuchen Zhang, Yanhe Zhang
SCIENCE August 19, 2005 (Vol. 309) ¹ NanoTech Institute University of Texas, USA & ² CSIRO (textile and fibre technology), Australia.
Advanced Manufacturing Choices
General Synthetic Scheme Tayo A. Sanders II, Mariah N. Sauceda, & Jennifer A. Dahl Nanoparticle Characterization Abstract  WiSys Technology Foundation.
Forging new generations of engineers. Properties of Materials.
Stress and Strain Unit 8, Presentation 1. States of Matter  Solid  Liquid  Gas  Plasma.
Carbon Nanotube Intramolecular Junctions. Nanotubes A graphene sheet with a hexagonal lattice…
 For many hundreds of years, diamond and graphite (Figure 1) were the only known crystalline allotropic forms of carbon. The discovery in the 1980’s.
Background about Carbon Nanotubes CAR Seminar 5 November 2010 Meg Noah.
Johnson Space Center May 18, Single-walled Carbon Nanotube (SWCNT) Carbon Nanostructures C 60 (Buckminsterfullerene)
PROPERTIES OF CARBON NANOTUBES
Chapter 21 Electromagnetic Waves. General Physics Exam II Curve: +30.
Design of Recuperative Heat Exchanger Presented by -- Jinying Zhu.
NSF NIRT Grant Hierarchical Nanomanufacturing of Carbon Nanotube Sheets and Yarns and their Applications for Active Nano-Materials Systems PIs:
Ductile Regime Machining of SiC J. Patten (PI), Western Michigan University, DMR We have previously demonstrated ductile regime machining of SiC.
CAREER: Synthesis and Electronic/Electrical Properties of Carbon Nanotube Junctions Wenzhi LiFlorida International UniversityDMR One of the objectives.
From Nanoscience to Nanomanufacturing STM manipulation of atoms 1989 AFM 1986 AFM manipulation of a SWNT 1999 Source: IBM Molecular logic gate 2002 Manipulation.
January 5, 2006 at Fermilab1 LAr TPC Wire Experiments B. Hansen.
National Science Foundation Novel Graphene-Fullerene Hybrid Materials: Experiment and Theory Krishna Muralidharan, University of Arizona, DMR Outcome:
IV. Results and Discussion Effect of Substrate Bias on Structure and Properties of W Incorporated Diamond-like Carbon Films Ai-Ying Wang 1, Kwang-Ryeol.
Super resolving pupils: beyond the diffraction limit * Anedio Ranfagni, Daniela Mugnai, Rocco Ruggeri In an attempt to transfer the results obtained with.
CARBON NANOTUBES By ANIKET KANSE
Carbon Nanotubes.
Measurement of Azimuthal Anisotropy for High p T Charged Hadrons at RHIC-PHENIX The azimuthal anisotropy of particle production in non-central collisions.
Namas Chandra and Sirish Namilae
I. Introduction  Carbon nanotubes (CNTs), composed of carbon and graphite sheets, are tubular shaped with the appearance of hexagonal mesh with carbon.
Carbon Nanotubes and Its Devices and Applications
Chapter 16 Lecture 2 Sheet Metal Forming. Figure 16.14a: Major Strain and Minor Strain During stretching in sheet metal, Volume constant –  l +  w +
Date of download: 6/22/2016 Copyright © ASME. All rights reserved. From: The Importance of Intrinsic Damage Properties to Bone Fragility: A Finite Element.
MESF593 Finite Element Methods
A Seminar presentation on
Derivatization of Carbon Nanotubes by the ZnO and ZnS nanoparticles
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Chapter X: Sheet Forming (Membrane Theory) 1 Content of Membrane Analysis Basic Assumptions Static Equilibrium Equations Strain State Application 1: Hole.
BDA30303 Solid Mechanics II.
POLYMERS Polymer Technology Thermoplastic Polymers
Ch. 2: Fundamental of Structure
Layered and scrolled nanocomposites with aligned semi-infinite graphene inclusions at the platelet limit by Pingwei Liu, Zhong Jin, Georgios Katsukis,
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Volume 105, Issue 10, Pages (November 2013)
Fig. 4 3D reconfiguration of liquid metals for electronics.
The Role of Network Architecture in Collagen Mechanics
GO-enabled templating synthesis of noble metal replicas.
Presentation transcript:

NSF NIRT Grant Hierarchical Nanomanufacturing of Carbon Nanotube Sheets and Yarns and their Applications for Active Nano-Materials Systems PIs: Ray H. Baughman, 1 Karen Lozano, 2 Anvar Zakhidov, 1 and Mei Zhang 3 1. University of Texas at Dallas, 2. University of Texas - Pan American, and 3. Florida State University I. Obtain and Deploy Deep Understanding of Sheet and Yarn Fabrication processes Fig. 1 (A) SEM image from movie showing the transformation of 300  m high nanotube forest (left) to nanotube sheet (right). (B) Schematic model of the fundamental process for the transformation of a nanotube forest (left) to a nanotube sheet, showing the critical role of nanotubes that migrate between bundles. Problem: Very few types of nanotube forests are drawable to make yarns and sheets, and minor changes in reaction conditions causes a transition from drawable forests to undrawable forests. Results:  Using movies of the drawing process taken in a SEM (Fig. 1A), a predictive model (Fig. 1B) explaining the transition from vertically aligned nanotubes in forests to horizontally aligned nanotubes in nanotube yarns and sheets was derived.  The nanotube bundle areal density and the linear density of inter-nanotube connections via migrant nanotubes were confirmed experimentally and theoretically to be key parameters needed for sheet or yarn drawability.  Increased nanotube length in spinable forests nearly ten fold, from 0.3 mm to 2.7 mm, by increasing nanotube diameter.  Synthesized nanotube forests having improved topology that enabled sheet draw at 120 m/minute and increased the width of drawable transparent sheets from 5 to 10 cm..  Demonstrated that false-twist and liquid-based densification provide comparable yarn strengths to those for twist-based spinning, and increased yarn strength to 1.2 GPa. II. Determine and Understand Sheet and Yarn Properties Results:  The measured thermal conductivity (3  method) of yarns (26 W/mK) and yarns (50 W/mK) is not high.  The strong observed dependence (Fig. 2) of thermal conductivity on nanotube bundling provides the explanation.  Inter-tube connections are relatively unimportant for limiting both phonon and electronic transport, since individual bundle and bulk measurements (normalized to density) differ little.  Network models indicate thermal and electrical transport on all walls of 8 wall, hundred  m long nanotubes.  Experiment and theory show mechanical stress transfer is low between outer and inner MWNT walls for above long nanotubes.  Individual MWNTs break, rather than slide out, when pulled from a twisted 10  m diameter yarn made of 8 wall, hundred  m long nanotubes.  Thermal expansion is negative at RT for twisted yarns (about -3.4X10 -6 /ºC).  Filtration-produced nanotube sheet shows abrupt switch in the sign of Poisson’s ratio vs. MWNT weight percent. Fig. 3 (A) Measured in-plane Poisson’s ratio (black) and density-normalized Young’s modulus (blue) vs. MWNT content in SWNT/MWNT sheets. The insert illustrates the effect of Poisson’s ratio sign on transverse curvature for a bent sheet strip. (B) Measured density-normalized tensile strength (black) and density (blue) vs. MWNT content in sheets. (C) Model for nanotube sheets, where meandering nanotubes are represented by zigzag chains. (D) The relationships between in-plane and thickness-direction Poisson’s ratios for SWNT (black) and MWNT (red) sheets having the force constant ratios R that yield the measured Poisson’s ratios (closed circles). The Poisson’s ratio changes result from varying the indicated average angle between the nanotubes and the sheet plane. Poisson’s ratios to the right of the blue line provide negative linear compressibilities. (Science 320, 504 (2008)). III. Demonstrate Sheet and Yarn Applications for Active Nano-Materials Systems Fig. 4 (Left) MRI imaging of a 3 mm mouse brain and 250  m blood vessel using carbon nanotube antenna, in collaborative work with Tursiop International (UTD licensee). (Right) Self- supporting 50 nm thick, transparent nanotube sheets mounted in metal frames for electron stripping in an ion beam accelerator. Results:  Demonstrated two new applications for MWNT sheets (Fig. 4), MRI antennas and transparent grids for electron stripping.  Demonstrated charge injection based carbon nanotube artificial muscles that operate between near 0 K and above 1900 K to provide over 3 X strokes in width and thickness directions, and over 10 4 %/s stroke rates IV. Demonstrate First Synthesis Route to Carbon Nanotubes of One Predetermined Type Fig. 5. A proposed synthesis route to carbon nanotubes of one type. Solid-state 1,4-addition polymerization reaction (A) converts linear stacks of cyclic tetradiyne molecules [-(CH 2 ) 4 C  C-C  C-] 4 (B) into a hydrocarbon nanotube (C), which is the proposed precursor to the (4,4) nanotube (D). Results  Two polymerizable tetramer phases were found, one with the tetramer rings skewered on an array of chloroforms.  Crystal structure determined (J. Reibenspies) for trimer phases and two tetramer phases - reactivity is consistent with theory.  When polymerizable, the expected Raman spectra and diffraction data for the hydrocarbon nanotube was obtained.  Conversion of the hydrocarbon nanotubes to nanotubes of one type has not yet been successful. AB Fig. 2. Thermal conductivity measurements on individual nanotube bundles show that bundling decreases thermal conductivity. A BCD AB