Tao Zheng Supervisor: Professor Harry Bhadeshia Richard Kemp

Slides:



Advertisements
Similar presentations
The Space Elevator and what we need to built it Photo source: space-elevator-and-become-an-interplanetary-civilization/
Advertisements

PHYSICS 231 INTRODUCTORY PHYSICS I
PH0101 UNIT 1 LECTURE 2 Shafts Torsion Pendulum-Theory and Uses
Thermoelastic properties of ferropericlase R. Wentzcovitch Dept. of Chemical Engineering and Materials Science, Minnesota Supercomputing Institute J. F.
Phy 212: General Physics II Chapter 20: Entropy & Heat Engines Lecture Notes.
Temperature Physics 202 Professor Lee Carkner Lecture 10.
THE WAVE EQUATION Alemayehu Adugna Arara Supervisor : Dr. J.H.M. ten Thije Boonkkamp November 04, 2009.
Thermo & Stat Mech - Spring 2006 Class 14 1 Thermodynamics and Statistical Mechanics Kinetic Theory of Gases.
POSCO Lectures on Bainite Graduate Institute of Ferrous Technology Microstructure Mechanism Properties Superbainite.
Mathematical Models and Novelty in Steels Tata Steel Jamshedpur.
37th John Player Memorial Lecture Design of strong, tough & affordable engineering alloys.
UPPER BAINITE (High Temperature) LOWER BAINITE (Low Temperature) Carbon supersaturated plate Carbon diffusion into austenite Carbon diffusion into austenite.
Transportable Classroom Table and Chair 1- Ahmed alshamrani 2- Mansour alrumayh 3- Abdulrahman alqadi 4-Ali alqadi 5-Mohannad alnufaie 6-Ahmed alobidy.
Viscous hydrodynamics and the QCD equation of state Azwinndini Muronga 1,2 1 Centre for Theoretical Physics and Astrophysics Department of Physics, University.
THE DISCOVERY, STRUCTURE, PROPERTIES AND APPLICATION OF CARBON NANOTUBES by Victoria Riabicheva Olexandra Tupalo English supervisor- Ekaterina Kuznetsova.
Conceptual Design of Continuous Processes for Carbon Nanotubes Adedeji E. Agboola and Ralph W. Pike Louisiana State University Helen H. Lou, Jack R. Hopper.
Cosires 2004 Helsinki June 28th – July 2nd Irradiation-induced stiffening of carbon nanotube bundles Maria Sammalkorpi (née Huhtala) 1, Arkady Krasheninnikov.
Glass Phenomenology from the connection to spin glasses: review and ideas Z.Nussinov Washington University.
Casing Integrity in Hydrate Bearing Sediments Reem Freij-Ayoub, Principal Research Engineer CESRE Wealth from Oceans.
DESIGN AND FABRICATION OF AN EXPERIMENTAL SETUP FOR SINGLE PLANE BALANCING Project Members- Nithin Seenivasan Nandaganesh M.R.Chitthaarth 8 th March, 2010.
11/03/2014PHY 711 Fall Lecture 291 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 29: Chap. 9 of.
Chapter 14: The Classical Statistical Treatment of an Ideal Gas.
Simulation Study of Magnetic Reconnection in the Magnetotail and Solar Corona Zhi-Wei Ma Zhejiang University & Institute of Plasma Physics Beijing,
“100 times stronger than steel” Iron is the standard against which life and new materials are compared Iron Lady Stalin Steely.
Investigation of flow distribution in multiple microchannels Reporter: Zhang Weihua Supervisor: Professor Xin Feng.
Spring Force and Energy Notes
First step in Understanding the Nature of Fluid Flow…. P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Analysis of Simplest Flow.
Hydrogen Storage and Pressure Increasing
Modelling of the motion of phase interfaces; coupling of thermodynamics and kinetics John Ågren Dept of Materials Science and Engineering Royal Institute.
CARBON NANOTUBES By ANIKET KANSE
Statistical physics in deformed spaces with minimal length Taras Fityo Department for Theoretical Physics, National University of Lviv.
Nanoclay minerals and plastics: tiny particles deliver big impact Suprakas Sinha Ray.
Analysis of Strain Effect in Ballistic Carbon Nanotube FETs
Chiara Di Paolo EN-STI-TCD Material Choice for the Vacuum Window at the Exit of BTM.
UNIT-01. SIMPLE STRESSES & STRAINS
Four-Stage of Engineering Analysis
Table 4. Mechanical properties of repair and substrate concrete
36th Dayton-Cincinnati Aerospace Sciences Symposium
3-D Printed Pressure Vessel Design to Maximize Volume to Weight
Trapping Modelling in MatCalc
Severly Deformed Steels
Date of download: 10/26/2017 Copyright © ASME. All rights reserved.
Evolution of Solutions Thermodynamics of mechanical alloying
Tensile strength (MPa) Length (m) of fibers/kg
Dr. Thomas Pozegic Prof. S. R. P. Silva Dr. I. Hamerton
Interplay of Modelling Techniques
Nanocrystalline Materials
Submitted by:- Paras Joshi R
M. Mahmoodi1, M. Arjmand2, U. Sundararaj2 and S. S. Park1
Poisons Ratio Poisons ratio = . w0 w Usually poisons ratio ranges from
Physics 202 Lecture 6 Thermodynamics.
Lecture 3: Other Ensembles and
Materials Science and Metallurgy Course A: Metals & Alloys
Class presentation to accompany reading of Chapter 2- Waves in Fluids
Materials Science and Metallurgy Mathematical Crystallography
Carbon Nanotube Diode Design
Evolution of Solutions Thermodynamics of Mechanical Alloying
R. Kemp, G. Cottrell and H. K. D. H. Bhadeshia
Supplement To Chapter 1 on OVERVIEW OF ENGINEERING ANALYSIS With additional information on Four-Stage of Engineering Analysis by Tai-Ran Hsu, Professor.
MIT Microstructural Evolution in Materials 8: Ionic Conductivity
Class presentation to accompany reading of Chapter 2- Waves in Fluids
Quasichemical Interstitial-Solutions: the carbon-carbon interaction energy Application of a first-order Quasichemical theory to Transformations in Steels,
The superconducting solenoids for the Super Charm-Tau Factory detector
PDT 153 Materials Structure And Properties
Lecture 11a Ideal gas Number of states and density of states
Budker Institute of Nuclear Physics,
Point and Path functions
Class presentation to accompany reading of Chapter 2- Waves in Fluids
Tutorial.
Mechanical Property 기계적 성질
Presentation transcript:

Tao Zheng Supervisor: Professor Harry Bhadeshia Richard Kemp Configurational Entropy as a function of Material Dimensions: A theory for strong ropes Tao Zheng Supervisor: Professor Harry Bhadeshia Richard Kemp

Outline space elevator. are carbon nanotube ropes ideal materials for space elevator project? 1 Configurational entropy 2 Stored energy and energy release rate 3 size-dependence of materials strength Conclusion

D.V.Smitherman 2005

High strength Lightweight > 62.5 GPa Carbon nanotubes Steel Kevlar Density 1300 kg m-3 7900 kg m-3 1440 kg m-3 Tensile strength 130 GPa < 5 GPa 3.6 GPa Bradley C. Edwards 2004

Steven L.Mielke et al (2004)

Equilibrium defect density Fromhold,Albert Thomas (1976)

Regular or ideal solution model Quasichemical solution model Lecture notes of Thermodynamics H K D H Bhadeshia (2004)

Energy release rate ( sound velocity): Stored energy Energy release rate ( sound velocity):

strength 130 GPa modulus 0.63 TPa Stored energy (J g-1) Energy release rate (m s-1) Dynamite 4650 6000 Nanotube 5420 21500 Bradley C. Edwards 2004

Different tensile strength value with different ropes length. Data from M.-F. Yu et al (2000); Min-Feng et al (2000); Z. W. Pan et al (1999)

Conclusion 1. By applying quasichemical solution model, more accurate configurational entropy and equilibrium defect density can be obtained. 2. Because of high strength and low density, carbon nanotubes have quite high stored energy and energy release rate which may make them not very safe in engineering application. 3. Strength of nanotube ropes will decrease sharply with increase of length of ropes.

Thank you!