Characterization and modeling to design and develop tailored-property filled glass composites

Size: px
Start display at page:

Download "Characterization and modeling to design and develop tailored-property filled glass composites"

Transcription

1 Engineering Conferences International ECI Digital Archives Composites at Lake Louise (CALL 2015) Proceedings Fall Characterization and modeling to design and develop tailored-property filled glass composites Kevin Ewsuk Sandia National Laboratories, Follow this and additional works at: Part of the Materials Science and Engineering Commons Recommended Citation Kevin Ewsuk, "Characterization and modeling to design and develop tailored-property filled glass composites" in "Composites at Lake Louise (CALL 2015)", Dr. Jim Smay, Oklahoma State University, USA Eds, ECI Symposium Series, (2016). This Conference Proceeding is brought to you for free and open access by the Proceedings at ECI Digital Archives. It has been accepted for inclusion in Composites at Lake Louise (CALL 2015) by an authorized administrator of ECI Digital Archives. For more information, please contact

2 Intensity 09:50 10:10 Louise Room Structural Composites Session I Photos placed in horizontal position with even amount of white space between photos and header Characterization and Modeling to Design and Develop Tailored-Property Filled-Glass Composites Kevin G. Ewsuk Sandia National Laboratories Albuquerque, NM Composites at Lake Louise-2015 November 8 12, 2015 Lake Louise, Alberta, Canada Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation, a wholly owned subsidiary of Lockheed Martin Corporation, for the U.S. Department of Energy s National Nuclear Security Administration under contract DE-AC04-94AL SAND NO XXXXP

3 Intensity Si-O Photos placed in horizontal position with even amount of white space between photos and header Al-O O-O Si-Si Al-Al Si-Al Ba-O Distance (Å) Todd R. Zeitler & Louise J. Criscenti - MD Modeling Michael T. Brumbach, Mark A. Rodriguez, & Todd M. Alam - Glass Structure Denise N. Bencoe & Bonnie McKenzie - Glass & Composite Characterization Sandia National Laboratories Richard K. Brow - Glass & Composite Characterization Missouri University of Science & Technology Karina Chapman - Glass Characterization Argonne National Laboratories Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation, a wholly owned subsidiary of Lockheed Martin Corporation, for the U.S. Department of Energy s National Nuclear Security Administration under contract DE-AC04-94AL SAND NO XXXXP

4 Glass Is Commonly Used To Bond/Join Inorganic Materials Glass bonding/joining Applications Glass-bonded composites Glass-bonded alumina Seals Hermetic glass-to-metal (GtM) seals Air bag igniters Medical implants Microelectronics Solid oxide fuel cells (SOFCs) *Feedthroughs for *Airbag igniter feedthroughs pressure & flow sensors *Schott Electronic Packaging 3

5 Filled-Glass Composites (FGCs) Have The Processability Of A Glass With The Properties Of A Ceramic Temp (ºC) Glass + Processability + Materials compatibility - Low/fixed CTE - Low toughness/crack tolerance Glass-Ceramic (GC) + Toughness/crack tolerance + High/Tunable CTE - Process sensitivity - Reactivity/Instability Li 3 PO 4 glass-like ceramic-like Li 2 SiO 4 SiO 2 Li 2 Si 2 O 5 Nucleation/Crystallization of different phases Time (min) Headley & Loehman, Crystallization of a Glass-Ceramic by Epitaxial Growth, J Am Ceram Soc, 67 [9] (1984). Filled-Glass Composite (FGC) + Process robustness + Toughness/Crack tolerance + Low to high/tunable CTE + Chemical/structural stability SS 60 mm SS GC GC 40 mm 4

6 Materials Science & Engineering Are Being Developed To Design/Develop Advanced Filled-Glass Composites Objectives Develop experimentally-validated modeling/simulation tools to: Predict/control glass chemistry-structure-property relations. Design & process filled-glass composites (FGCs). Approach Characterize & model glass chemistry-structure-property relations. Predict glass chemistry-structure relations with MD modeling. Characterize glass chemistry-structure (NN distance & NMR peak shifts). Characterize & model FGC processing & properties. Design FGCs using mixing models. Characterize glass & FGC wetting/interactions on stainless steel (SS). Characterize glass & FGC viscosity for process modeling. Test, refine, & validate modeling/simulation by comparison to experiment 5

7 BAS Glasses Were Simulated With The LAMMPS** MD Code & Pedone* Multicomponent Force Field BAS 1 25 BaO X Al 2 O 3 (75-x) SiO 2 Glasses BAS 2 BAS 3 25 BaO - 75 SiO 2 25 BaO - 5 Al 2 O 3-70 SiO 2 25 BaO - 15 Al 2 O 3-60 SiO 2 T. Zeitler *A Pedone et al., A new self-consistent empirical interatomic potential model for oxides, silicates, and silica-based glasses, J Phys Chem B, 110, (2006). **S Plimpton, Fast Parallel Algorithms for Short-Range Molecular-Dynamics, J Comp Phys, 117 [1], 1-19 (1995). 6

8 Intensity Model Predictions Of Chemistry-Structure Relations Were Tested & Validated By Comparison To Theory % % Glass g/mole Mole % Al 2 O 3 NBO Th (%) NBO MD (%) Connectivity Th (BO/NF) BAS BAS BAS BAS T. Zeitler Peak position & symmetry increase from BAS 1 3 Si-O-Si Q 4 /Q 3 increases from BAS 1 3 (with decreasing NBOs) BOs:NBOs increases from BAS 1 3 BAS 1 BAS 2 BAS Bond Angle (Å) CN BO NBO TBO Oxygen Speciation 7

9 Model Predictions Of Glass Chemistry-Structure Were Tested & Validated By Comparison To Experiment Tool Nearest Neighbor (NN) Distances NN Assignments Coordination Number (CN) Model Y Y Y apdf NMR Y Trends for Si & Al Inferred from crystallography Non-Bridging Oxygens (NBOs) Bond Angle Distributions, BO s/ NBO s Order/Disorder Trends Glasses BAS 1-3,8 BAS 1-3,8 BAS 1-3,8 EXAFS Y Y (Ba) Y (Ba) BAS 1-3,8 8

10 Intensity Intensity Measured apdf Peaks Are Consistent With Nearest Neighbor (NN) Distances From MD Simulations Si-O Al-O O-O Si-Si Al-Al Si-Al Ba-O Si-O Al-O O-O Ba-O Si-O Al-O BAS 1 BAS 2 BAS 3 G (r) Distance (Å) 1 st 2 nd 3 rd 4th 5 th Synchrotron apdf analysis l = Å Q max = 21 Å -1. Atomic Pair Distribution Functions (apdfs) - K. Chapman - Argonne 1 2 Nearest 3 Neighbor (NN) 4 distance (Å) 5 NN distance (Angstroms) Distance (Å) MD simulation T. Zeitler BAS 7 BAS 6 BAS 5 BAS 3 BAS 2 BAS 1 BAS 8 1 st - Si-O & Al-O 2 nd - O-Si-O 3 rd - Ba-O 4 th - O-Si-O-Si 5 th - O-Al-O-Si-O Ba-Ba M. Rodriguez 9

11 29 Si MAS-NMR Q 3 & Q 4 Peaks Are Accurately Predicted From MD Coordinates, But The Q 3 :Q 4 Ratio Differs Si(OSi) 4 d = ppm Si(OSi) 3 Al d = ppm Si(OSi) 3 Ba d = ppm NMR Calculated 29 Si chemical shifts using MD coordinates. Employed correlation from Sherrif et al. (1991) based on silicate mineral structures. Factors included bond valence (s i ), angle of the bridging oxygen, Si-O bond distance, and distance to the 2 nd nearest neighbors. si exp r0 ri / 0.37 Calculation N i 1 s R D 2 3 i 1 3cos i / 3 i log i 29 d ( Si) T. Alam 29 Si Chemical Shift (ppm) 10

12 MD Simulations Show A Higher Relative Concentration Of Glass Network Modifiers On The Glass Surface K T-1 O Si Al Co O T-1 (modified) Si Al T. Zeitler 11

13 Filled-Glass Composite (FGC) Properties Are Consistent With Model Predicted Trends Viscosity (Pa s) ΔL/L o dl/ Lo * Temper at ur e / C M a i n : 5 7 U s e r : E D [ # ] I n... F50 i l e 100 D a t e I d e n t i150 t y S a mp l e 200 L... S.. R. a n250 g e A t mo s p h300 e r e [ 4. 1 ]... [ 4. 2 ]... [ 5. 1 ]... [ 5. 2 ]... [ 6. 1 ]... [ 6. 2 ]... CGI % quar t z Temp. / C 50. 0, : Temp. / C 50. 0, : C G I _ B L U... C G I _ B L U... C G I %... C G I %... C G I %... C G I %... T. Al pha/ ( 1/ K) E- 06 T. Al pha/ ( 1/ K) E Material F E mo d e... F E mo d e... C G I B u m q t z C G I Temperature 1 0 u m q t z C G I ( C) u m q t z 1 0 u m q t z 10v% FGC 10.5 E-6 in/in/c CGI % quar t z Temp. / C T. Al pha/ ( 1/ K) 50. 0, : E- 06 Temp. / C 50. 0, : C G I B... C G I C G I T. Al pha/ ( 1/ K) E- 06 Glass 9.9 E-6 in/in/c Measured CTE (ppm/c) Predicted CTE (ppm/c) Glass v% FGC v% FGC v% FGC 11.0 E-6 in/in/c CGI gl ass Temp. / C 50. 0, : Temp. / C 50. 0, : / 1. 0 ( / / 1. 0 ( / / 1. 0 ( / T. Al pha/ ( 1/ K) E- 06 T. Al pha/ ( 1/ K) E- 06 [ [ ] ] D. Bencoe n i t r o g e n / 6 0 / n i t r o g e n / 6 0 / n i t r o g e n / 6 0 / n i t r o g e n / 6 0 / n i t r o g e n / 6 0 / n i t r o g e n / 6 0 / [ 5. 2 ] 1 [[ ]] C E+10 1.E+09 1.E+08 1.E+07 Glass 10v% FGC 1.E Temperature ( C) Euler s Model R. Brow MO U S&T 12

14 Viscosity Data Will Enable The Use Of Process Modeling To Optimize FGC Designs For Manufacturability Euler s Model FGC Process Map NLPS Model Ewsuk & Harrison, Ceramic Trans,

15 Sessile Drop Experiments Were Completed On Stainless Steel To Characterize Wetting & Viscous Flow Thermocouple Stainless Steel Glass (left) Composite (right) R. Brow MO U S&T 14

16 Sessile Drop Data Were Analyzed To Better Quantify Differences In Viscous Behavior 1. First shrinkage or sintering: Temperature pressed sample starts to shrink (logh=10 0±0 3 P). 2. Point of maximum shrinkage: Temperature of maximum sample shrinkage before it starts to soften (logh=8 2±0 5 P). 3. Softening point: Temperature of first signs of softening (disappearance or rounding of edges of the sample (logh=6 1±0 2 P). 4. Half ball point: Temperature at which sample forms a (logh=4 6±0 1 P). 5. Flow point: Temperature of maximum height of the drop of molten glass (logh= P). Scholze, Influence of viscosity and surface tension on hot-stage microscopy measurements on glasses, Ver. Dtsch. Keram. Ges., 1962, 391, 63 8.) Softening Point Half Ball Point Flow Point Pascual, et al., Phys. Chem. Glasses (2001) 42[1]

17 The Filler Addition Increases FGC Viscosity And Decrease FGC Reactivity Relative To The Glass Interaction Zone h/h Glass Stable melt temp: 915 C 935 C First shrinkage temp: 590 C 620 C 10v% FGC Half height temp: 767 C 825 C SS Interface R. Brow MO U S&T B. McKenzie 10v% FGC Glass ~100 mm Zone ~130 mm Zone 60 mm 60 mm 16

18 Oxidizing The Stainless Steel Enhances Initial Wetting And Reaction FGC composite H/H o SS Interface Wetting on SS Glass 10V% FGC Temperature/C Wetting on Oxidized SS R. Brow MO U S&T Glass 10V% FGC Temperature/C B. McKenzie ~80 mm interaction zone 60 mm 60 mm 17

19 Experimentally-Validated Modeling Is Being Developed To Enable Advanced FGC Design And Fabrication Summary Characterized & Modeled Glass Chemistry-Structure. Good modelling-experiment first-order agreement. MD efficient to assess bulk glass chemistry-structure. Interface modeling consistent with expectations Higher surface concentration of network modifiers. Characterized & Modeled FGC Properties & Processing. Measured CTE & viscosity trend as predicted by modeling. Wetting & reactivity are consistent with expectations Higher viscosity & lower reactivity FGCs relative to glass. Initial wetting & reactivity are enhanced on oxidized SS. 18

Ceramic Engineering 103 Final Exam (5/16/03) 1) Arrange each set of oxides in order from most basic to most acidic (3 points each):

Ceramic Engineering 103 Final Exam (5/16/03) 1) Arrange each set of oxides in order from most basic to most acidic (3 points each): Cer 103 Final Exam/WS03 (2) Test 5 030516 3) Sketch a TTT curve for a system containing 0.1 vol% of crystalline material. Add a second curve for 1 vol% crystallinity. Label both curves and label each axis.

More information

Wolter Imaging On Z. Chris Bourdon, Manager Z Imaging and Spectroscopy Julia Vogel, LLNL; Ming Wu, SNL ICF Diagnostics Workshop, October 5 th 2015

Wolter Imaging On Z. Chris Bourdon, Manager Z Imaging and Spectroscopy Julia Vogel, LLNL; Ming Wu, SNL ICF Diagnostics Workshop, October 5 th 2015 Photos placed in horizontal position with even amount of white space between photos and header Wolter Imaging On Z Chris Bourdon, Manager Z Imaging and Spectroscopy Julia Vogel, LLNL; Ming Wu, SNL ICF

More information

Glass Transformation-Range Behavior- Odds and Ends

Glass Transformation-Range Behavior- Odds and Ends Web Course Physical Properties of Glass Glass Transformation-Range Behavior- Odds and Ends Richard K. Brow Missouri University of Science & Technology Department of Materials Science & Engineering Glass

More information

Growth of Graphene Architectures on SiC

Growth of Graphene Architectures on SiC Wright State University CORE Scholar Special Session 5: Carbon and Oxide Based Nanostructured Materials (2012) Special Session 5 6-2012 Growth of Graphene Architectures on SiC John J. Boeckl Weijie Lu

More information

Optimal molecular design of poly (ionic liquids) for CO2 capture from the atmosphere

Optimal molecular design of poly (ionic liquids) for CO2 capture from the atmosphere Engineering Conferences International ECI Digital Archives CO2 Summit II: Technologies and Opportunities Proceedings Spring 4-13-2016 Optimal molecular design of poly (ionic liquids) for CO2 capture from

More information

Competitive I 2 Sorption by Cu-BTC from Humid Gas Streams

Competitive I 2 Sorption by Cu-BTC from Humid Gas Streams Supporting Information for: Competitive I 2 Sorption by Cu-BTC from Humid Gas Streams Dorina F. Sava, Karena W. Chapman, Mark A. Rodriguez, Jeffery A. Greathouse, # Paul S. Crozier,^ Haiyan Zhao, Peter

More information

DECRIRE LA TRANSITION VITREUSE: Simulations moléculaires et approches topologiques. Matthieu Micoulaut, LPTMC, Paris Sorbonne Universités UPMC

DECRIRE LA TRANSITION VITREUSE: Simulations moléculaires et approches topologiques. Matthieu Micoulaut, LPTMC, Paris Sorbonne Universités UPMC DECRIRE LA TRANSITION VITREUSE: Simulations moléculaires et approches topologiques Matthieu Micoulaut, LPTMC, Paris Sorbonne Universités UPMC C. Yildrim, O. Laurent, B. Mantisi, M. Bauchy «Chasseurs d

More information

Rheology, Adhesion, and Debonding of Lightly Cross-linked Polymer Gels

Rheology, Adhesion, and Debonding of Lightly Cross-linked Polymer Gels Rheology, Adhesion, and Debonding of Lightly Cross-linked Polymer Gels Nicholas B. Wyatt, and Anne M. Grillet 2 Materials Science and Engineering Division 2 Engineering Sciences Division Sandia National

More information

High-Pressure Equation of State of Cesium Fluoride to 120 GPa

High-Pressure Equation of State of Cesium Fluoride to 120 GPa Proc. 17th Int. Conf. on High Pressure in Semiconductor Physics & Workshop on High-pressure Study on Superconducting JJAP Conf. Proc. 6, https://doi.org/10.7567/jjapcp.6.011101 High-Pressure Equation of

More information

Characterization of wind velocity distributions within a full-scale heliostat field

Characterization of wind velocity distributions within a full-scale heliostat field Photos placed in horizontal position with even amount of white space between photos and header Characterization of wind velocity distributions within a full-scale heliostat field Jeremy Sment, Graduate

More information

Three-Dimensional Silicon Photonic Crystals

Three-Dimensional Silicon Photonic Crystals Three-Dimensional Silicon Photonic Crystals Shawn-Yu Lin'*, J. G. Fleming', D.L. Hetherington', B.K. Smith', W. Zubrzycki', R. Biswas2, M.M. Sigalas2, and K.M. Ho2. 'Sandia National Laboratories, P.O.

More information

Chapter 2. Atomic Structure

Chapter 2. Atomic Structure Chapter 2 Atomic Structure 2 6 (a) Aluminum foil used for storing food weighs about 0. g per square cm. How many atoms of aluminum are contained in one 6.25 cm 2 size of foil? (b) Using the densities and

More information

Chapter Outline: Ceramics. Chapter 13: Structure and Properties of Ceramics

Chapter Outline: Ceramics. Chapter 13: Structure and Properties of Ceramics Chapter Outline: Ceramics Chapter 13: Structure and Properties of Ceramics Crystal Structures Silicate Ceramics Carbon Imperfections in Ceramics Optional reading: 13.6 13.10 University of Virginia, Dept.

More information

Make sure the exam paper has 9 pages (including cover page) + 3 pages of data for reference

Make sure the exam paper has 9 pages (including cover page) + 3 pages of data for reference UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences Spring 2006 EE143 Midterm Exam #1 Family Name First name SID Signature Make sure the exam paper

More information

A CFD study of gas-solid separation in a downer pyrolysis reactor: An eulerian-eulerian approach

A CFD study of gas-solid separation in a downer pyrolysis reactor: An eulerian-eulerian approach Engineering Conferences International ECI Digital Archives BioEnergy IV: Innovations in Biomass Conversion for Heat, Power, Fuels and Chemicals Proceedings Spring 6-10-2013 A CFD study of gas-solid separation

More information

Chapter 10: Liquids and Solids

Chapter 10: Liquids and Solids Chapter 10: Liquids and Solids Chapter 10: Liquids and Solids *Liquids and solids show many similarities and are strikingly different from their gaseous state. 10.1 Intermolecular Forces Intermolecular

More information

Chapter 12: Structures & Properties of Ceramics

Chapter 12: Structures & Properties of Ceramics Chapter 12: Structures & Properties of Ceramics ISSUES TO ADDRESS... How do the crystal structures of ceramic materials differ from those for metals? How do point defects in ceramics differ from those

More information

Photos placed in horizontal position with even amount of white space between photos and header

Photos placed in horizontal position with even amount of white space between photos and header Photos placed in horizontal position with even amount of white space between photos and header XPCA: Copula-based Decompositions for Ordinal Data Clifford Anderson-Bergman, Kina Kincher-Winoto and Tamara

More information

Photos placed in horizontal p osition with even amount of white sp ace between photos and header

Photos placed in horizontal p osition with even amount of white sp ace between photos and header Photos placed in h orizontal position with even amount of white space between photos a nd header Interbed Modeling to Predict Wellbore Damage for ig Hill Strategic Petroleum Reserve Photos placed in horizontal

More information

Lecture 8 Chemical/Electronic Structure of Glass

Lecture 8 Chemical/Electronic Structure of Glass Lecture 8 Chemical/Electronic Structure of Glass Syllabus Topic 6. Electronic spectroscopy studies of glass structure Fundamentals and Applications of X-ray Photoelectron Spectroscopy (XPS) a.k.a. Electron

More information

Chapter 12: Structures & Properties of Ceramics

Chapter 12: Structures & Properties of Ceramics Chapter 12: Structures & Properties of Ceramics ISSUES TO ADDRESS... Structures of ceramic materials: How do they differ from those of metals? Point defects: How are they different from those in metals?

More information

High Temperature Water Clean and Etch Reactions with Low-k and SiO 2 Films: Experiments and Simulations

High Temperature Water Clean and Etch Reactions with Low-k and SiO 2 Films: Experiments and Simulations High Temperature Water Clean and Etch Reactions with Low-k and SiO 2 Films: Experiments and Simulations Joshua Barclay, Lu Deng, Oseoghaghare Okobiah, Tina Sengphanlaya, Jincheng Du, Rick Reidy University

More information

Atomistic structure of calcium silicate intergranular films between prism and basal planes in silicon nitride: A molecular dynamics study

Atomistic structure of calcium silicate intergranular films between prism and basal planes in silicon nitride: A molecular dynamics study Atomistic structure of calcium silicate intergranular films between prism and basal planes in silicon nitride: A molecular dynamics study Xiaotao Su and Stephen H. Garofalini Department of Ceramics and

More information

Kinetic enhancement of adsorbent for CO2 capture from atmosphere by porous material

Kinetic enhancement of adsorbent for CO2 capture from atmosphere by porous material Engineering Conferences International ECI Digital Archives CO2 Summit II: Technologies and Opportunities Proceedings Spring 4-13-2016 Kinetic enhancement of adsorbent for CO2 capture from atmosphere by

More information

An overview of the. package for non-conformal mesh tying or simple contact problems

An overview of the. package for non-conformal mesh tying or simple contact problems An overview of the package for non-conformal mesh tying or simple contact problems Glen Hansen 2012 Trilinos User Group Meeting Oct. 30, 2012 SAND 2012-9202P (UUR) Sandia National Laboratories is a multi-program

More information

Quantum Hall Effect in Vanishing Magnetic Fields

Quantum Hall Effect in Vanishing Magnetic Fields Quantum Hall Effect in Vanishing Magnetic Fields Wei Pan Sandia National Labs Sandia is a multi-mission laboratory operated by Sandia Corporation, a Lockheed Martin Company, for the United States Department

More information

Chapter 10 Liquids and Solids. Problems: 14, 15, 18, 21-23, 29, 31-35, 37, 39, 41, 43, 46, 81-83, 87, 88, 90-93, 99, , 113

Chapter 10 Liquids and Solids. Problems: 14, 15, 18, 21-23, 29, 31-35, 37, 39, 41, 43, 46, 81-83, 87, 88, 90-93, 99, , 113 Chapter 10 Liquids and Solids Problems: 14, 15, 18, 21-23, 29, 31-35, 37, 39, 41, 43, 46, 81-83, 87, 88, 90-93, 99, 104-106, 113 Recall: Intermolecular vs. Intramolecular Forces Intramolecular: bonds between

More information

Glass V.M. Sglavo GlassEng - UNITN 2017

Glass V.M. Sglavo GlassEng - UNITN 2017 Glass Definition material with no long range order matarial characterized by the glass transition phenomenon amorphous solid without long range order and ordered atomic structure, which shows the glass

More information

Stochastic Generation Expansion Planning

Stochastic Generation Expansion Planning Engineering Conferences International ECI Digital Archives Modeling, Simulation, And Optimization for the 21st Century Electric Power Grid Proceedings Fall 10-23-2012 Stochastic Generation Expansion Planning

More information

The effect of extended strain fields on point defect scattering

The effect of extended strain fields on point defect scattering Engineering Conferences International ECI Digital Archives Nonstoichiometric Compounds VI Proceedings 9-8-2016 The effect of extended strain fields on point defect scattering Brenden R. Ortiz Colorado

More information

Drilling And Testing in the Deep Borehole Field Test

Drilling And Testing in the Deep Borehole Field Test Photos placed in horizontal position with even amount of white space between photos and header Drilling And Testing in the Deep Borehole Field Test Kristopher L. Kuhlman, David C. Sassani, Geoff A. Freeze,

More information

Density, Volume, and Packing: Part 2 Thursday, September 4, 2008 Steve Feller Coe College Physics Department

Density, Volume, and Packing: Part 2 Thursday, September 4, 2008 Steve Feller Coe College Physics Department Density, Volume, and Packing: Part 2 Thursday, September 4, 2008 Steve Feller Coe College Physics Department Lecture 3 of Glass Properties Course Some Definitions x = molar fraction of alkali or alkaline-earth

More information

Effects of ph on the Gelation Time in the Sol-Gel Polymerization of 1,6-Bis(trimethoxysiIy I)hexane

Effects of ph on the Gelation Time in the Sol-Gel Polymerization of 1,6-Bis(trimethoxysiIy I)hexane Effects of ph on the Gelation Time in the Sol-Gel Polymerization of 1,6-Bis(trimethoxysiy )hexane ph 1-13 Buffered Constant onic Strength 6 M Douglas A b y *, Brian Mather?, Andrei R Straumanisf, Colleen

More information

The Science and Engineering of Materials, 4 th ed Donald R. Askeland Pradeep P. Phulé. Chapter 2 Atomic Structure

The Science and Engineering of Materials, 4 th ed Donald R. Askeland Pradeep P. Phulé. Chapter 2 Atomic Structure The Science and Engineering of Materials, 4 th ed Donald R. Askeland Pradeep P. Phulé Chapter 2 Atomic Structure Objectives of Chapter 2 The goal of this chapter is to describe the underlying physical

More information

Nonlinearity of Joints in Structural Dynamics of Weapons Systems

Nonlinearity of Joints in Structural Dynamics of Weapons Systems Nonlinearity of Joints in Structural Dynamics of Weapons Systems Daniel Brown AWE Dan Segalman Sandia National Laboratories Sandia National Laboratories is a multi-program laboratory managed and operated

More information

ANSWER KEY. SECOND MIDTERM EXAM Chemistry April 2011 Professor Buhro

ANSWER KEY. SECOND MIDTERM EXAM Chemistry April 2011 Professor Buhro ANSWER KEY SECOND MIDTERM EXAM Chemistry 465 12 April 2011 Professor Buhro ANSWER KEY Signature ANSWER KEY Print Name Clearly ID Number: Information. This is a closed-book exam; no books, notes, other

More information

Chapter 3. The structure of crystalline solids 3.1. Crystal structures

Chapter 3. The structure of crystalline solids 3.1. Crystal structures Chapter 3. The structure of crystalline solids 3.1. Crystal structures 3.1.1. Fundamental concepts 3.1.2. Unit cells 3.1.3. Metallic crystal structures 3.1.4. Ceramic crystal structures 3.1.5. Silicate

More information

Multiphysics modeling of thermal batteries

Multiphysics modeling of thermal batteries Multiphysics modeling of thermal batteries Scott A. Roberts, Ph.D. Thermal/Fluid Component Sciences Department Sandia National Laboratories, Albuquerque, NM The Future of Munitions Batteries Workshop Army

More information

Integration of Boiling Experiments in the Undergraduate Heat Transfer Laboratory

Integration of Boiling Experiments in the Undergraduate Heat Transfer Laboratory Integration of Boiling Experiments in the Undergraduate Heat Transfer Laboratory Hosni I. Abu-Mulaweh, Josué Njock Libii Engineering Department Indiana University-Purdue University at Fort Wayne Fort Wayne,

More information

Sol-Gel Methods. Hydrolysis Condensation Gelation Ageing Drying Densification

Sol-Gel Methods. Hydrolysis Condensation Gelation Ageing Drying Densification Sol-Gel Methods Sol-gel process: Hydrolysis Condensation Gelation Ageing Drying Densification Powders: microcrystalline, nanocrystalline, amorphous Monoliths, Coatings, Films, Fibers Aerogels Glasses,

More information

DSMC-Based Shear-Stress/Velocity-Slip Boundary Condition for Navier-Stokes Couette-Flow Simulations

DSMC-Based Shear-Stress/Velocity-Slip Boundary Condition for Navier-Stokes Couette-Flow Simulations DSMC-Based Shear-Stress/Velocity-Slip Boundary Condition for Navier-Stokes Couette-Flow Simulations J. R. Torczynski and M. A. Gallis Engineering Sciences Center, Sandia National Laboratories, P. O. Box

More information

Miguel Aguilo, Ted Blacker, Andre Claudet, Brett Clark, Ryan Rickerson, Josh Robbins, Louis Vaught, and Tom Voth Sandia National Laboratories

Miguel Aguilo, Ted Blacker, Andre Claudet, Brett Clark, Ryan Rickerson, Josh Robbins, Louis Vaught, and Tom Voth Sandia National Laboratories Miguel Aguilo, Ted Blacker, Andre Claudet, Brett Clark, Ryan Rickerson, Josh Robbins, Louis Vaught, and Tom Voth (as told by Corbett Battaile) Sandia National Laboratories Sandia National Laboratories

More information

Hydrogeology of Deep Borehole Disposal for High-Level Radioactive Waste

Hydrogeology of Deep Borehole Disposal for High-Level Radioactive Waste SAND2014-18615C Hydrogeology of Deep Borehole Disposal for High-Level Radioactive Waste Geological Society of America Annual Meeting October 20, 2014 Bill W. Arnold, W. Payton Gardner, and Patrick V. Brady

More information

Multiphysics Modeling of Pre-ignition Damage in Energetic Materials and the Effect on Cookoff Violence

Multiphysics Modeling of Pre-ignition Damage in Energetic Materials and the Effect on Cookoff Violence Multiphysics Modeling of Pre-ignition Damage in Energetic Materials and the Effect on Cookoff Violence Dan Turner dzturne@sandia.gov Department of Thermal & Fluid Mechanics Sandia National Laboratories

More information

3.032 Problem Set 4 Fall 2007 Due: Start of Lecture,

3.032 Problem Set 4 Fall 2007 Due: Start of Lecture, 3.032 Problem Set 4 Fall 2007 Due: Start of Lecture, 10.19.07 1. A microelectronic sensor is to be made of conductive wires deposited on a thin Si wafer. During design considerations, it was decided that

More information

Chapter 12: Structures of Ceramics

Chapter 12: Structures of Ceramics Chapter 12: Structures of Ceramics Outline Introduction Crystal structures Ceramic structure AX-type crystal structures A m X p -type A m B n X p - type Silicate ceramics Carbon Chapter 12 - Ceramics Two

More information

LITHIUM COORDINATION MEASUREMENT IN THE LITHIUM DISILICATE GLASSES

LITHIUM COORDINATION MEASUREMENT IN THE LITHIUM DISILICATE GLASSES Romanian Reports in Physics, Volume 56, No. 3, P. 413-418, 2004 LITHIUM COORDINATION MEASUREMENT IN THE LITHIUM DISILICATE GLASSES D. RADU 1, C. MAZILU 2, B. GRIGORAS 2 1 University Politehnica Bucharest,

More information

Detection and relevance of ion conduction in hybrid organic-inorganic halide perovskites for photovoltaic applications

Detection and relevance of ion conduction in hybrid organic-inorganic halide perovskites for photovoltaic applications Engineering Conferences International ECI Digital Archives Nonstoichiometric Compounds VI Proceedings 9-7-2016 Detection and relevance of ion conduction in hybrid organic-inorganic halide perovskites for

More information

Coupling of Multi fidelity Models Applications to PNP cdft and local nonlocal Poisson equations

Coupling of Multi fidelity Models Applications to PNP cdft and local nonlocal Poisson equations Coupling of Multi fidelity Models Applications to PNP cdft and local nonlocal Poisson equations P. Bochev, J. Cheung, M. D Elia, A. Frishknecht, K. Kim, M. Parks, M. Perego CM4 summer school, Stanford,

More information

Parallel Simulation of Subsurface Fluid Flow

Parallel Simulation of Subsurface Fluid Flow Parallel Simulation of Subsurface Fluid Flow Scientific Achievement A new mortar domain decomposition method was devised to compute accurate velocities of underground fluids efficiently using massively

More information

Ceramic Processing Research

Ceramic Processing Research Journal of Ceramic Processing Research. Vol. 9, 4, pp. 401~406 (2008) J O U R N A L O F Ceramic Processing Research Studies on the characterization of sulfur and coloration in borosilicate glasses Taro

More information

Characterizing and Modeling Wind Power Forecast Errors from Operational Systems for Use in Wind Integration Planning Studies

Characterizing and Modeling Wind Power Forecast Errors from Operational Systems for Use in Wind Integration Planning Studies Engineering Conferences International ECI Digital Archives Modeling, Simulation, And Optimization for the 21st Century Electric Power Grid Proceedings Fall 10-23-2012 Characterizing and Modeling Wind Power

More information

Density. Physical Properties of Materials. Which Ones? THEORETICAL DENSITY, ρ. What would make a material dense? Concept Question. Physical Properties

Density. Physical Properties of Materials. Which Ones? THEORETICAL DENSITY, ρ. What would make a material dense? Concept Question. Physical Properties Physical Properties of Materials Let s get physical!! density Physical Properties electrical thermal expansion shock Density Which Ones? melting point What is density? = THEORETICAL DENSITY, ρ Concept

More information

Structural characterization begins with a purity check!

Structural characterization begins with a purity check! Structural characterization begins with a purity check! Refractive Index Melting Point Elemental Analysis (EA) Thin Layer Chromatography (TLC) High Performance Liquid Chromatography (HPLC) Course: 59-320

More information

Predicting Mineral Transformations in Wet Supercritical CO 2 : The Critical Role of Water

Predicting Mineral Transformations in Wet Supercritical CO 2 : The Critical Role of Water Predicting Mineral Transformations in Wet Supercritical CO 2 : The Critical Role of Water Andrew R. Felmy Eugene S. Ilton Andre Anderko Kevin M. Rosso Ja Hun Kwak Jian Zhi Hu 1 Outline Background Importance

More information

X-ray Spectroscopy. Lecture plan. A Critical Look at the Past Accomplishments and Future Prospects. Proposal body not more than 5 pages

X-ray Spectroscopy. Lecture plan. A Critical Look at the Past Accomplishments and Future Prospects. Proposal body not more than 5 pages X-ray Spectroscopy A Critical Look at the Past Accomplishments and Future Prospects James Penner-Hahn jeph@umich.edu Room 243 Monday Wednesday 3-5 PM and by appointment http://www.chem.usyd.edu.au/~penner_j/index.htm

More information

ntof (and other) measurements at Z:

ntof (and other) measurements at Z: ntof (and other) measurements at Z: Assessing the impacts of flows, spatial variations, and Magnetic Fields Patrick Knapp NISP Working Group LLNL, Livermore CA March 8, 2016 Photos placed in horizontal

More information

P. W. Anderson [Science 1995, 267, 1615]

P. W. Anderson [Science 1995, 267, 1615] The deepest and most interesting unsolved problem in solid state theory is probably the theory of the nature of glass and the glass transition. This could be the next breakthrough in the coming decade.

More information

Molecular dynamics simulation of lithium diffusion in Li 2 O Al 2 O 3 SiO 2 glasses

Molecular dynamics simulation of lithium diffusion in Li 2 O Al 2 O 3 SiO 2 glasses Solid State Ionics 166 (2004) 365 373 www.elsevier.com/locate/ssi Molecular dynamics simulation of lithium diffusion in Li 2 O Al 2 O 3 SiO 2 glasses Weiqun Li, Stephen H. Garofalini* Department of Ceramic

More information

First Shell EXAFS Analysis

First Shell EXAFS Analysis EXAFS Data Collection and Analysis Workshop, NSLS, July, First Shell EXAFS Analysis Anatoly Frenkel Physics Department, Yeshiva University, New York, NY 116 frenkel@bnl.gov General strategy: -Collect good

More information

SYNTHESIS OF INORGANIC MATERIALS AND NANOMATERIALS. Pr. Charles Kappenstein LACCO, Laboratoire de Catalyse en Chimie Organique, Poitiers, France

SYNTHESIS OF INORGANIC MATERIALS AND NANOMATERIALS. Pr. Charles Kappenstein LACCO, Laboratoire de Catalyse en Chimie Organique, Poitiers, France SYNTHESIS OF INORGANIC MATERIALS AND NANOMATERIALS Pr. Charles Kappenstein LACCO, Laboratoire de Catalyse en Chimie Organique, Poitiers, France Outline IV - FORMATION OF SOLIDS FROM SOLUTIONS 1) Glass

More information

A STUDY OF THERMAL PROPERTIES OF PEROVSKITE CERAMIC MATERIALS VIA MOLECULAR DYNAMICS SIMULATION

A STUDY OF THERMAL PROPERTIES OF PEROVSKITE CERAMIC MATERIALS VIA MOLECULAR DYNAMICS SIMULATION A STUDY OF THERMAL PROPERTIES OF PEROVSKITE CERAMIC MATERIALS VIA MOLECULAR DYNAMICS SIMULATION Wen Fong Goha*, Sohail Aziz Khana and Tiem Leong Yoona School of Physics, Universiti Sains Malaysia, 11800,

More information

Encapsulation of biological materials

Encapsulation of biological materials Engineering Conferences International ECI Digital Archives Design and Manufacture of Functional Microcapsules and Engineered Products Proceedings 4-5-2016 Encapsulation of biological materials Alexander

More information

Chap 10 Part 3a.notebook December 12, 2017

Chap 10 Part 3a.notebook December 12, 2017 Metallic Bonding and Semiconductors Chapter 10 Sect 4 Metallic Bonding positive metal ions surrounded by a "sea of electrons" Bonding is strong and nondirectional Iron, Silver, alloys, Brass, Bronze Forces

More information

Title Single Row Nano-Tribological Printing: A novel additive manufacturing method for nanostructures

Title Single Row Nano-Tribological Printing: A novel additive manufacturing method for nanostructures Nano-Tribological Printing: A novel additive manufacturing method for nanostructures H.S. Khare, N.N. Gosvami, I. Lahouij, R.W. Carpick 1 Mechanical Engineering and Applied Mechanics, University of Pennsylvania,

More information

Lecture 4! ü Review on atom/ion size! ü Crystal structure (Chap 4 of Nesseʼs book)!

Lecture 4! ü Review on atom/ion size! ü Crystal structure (Chap 4 of Nesseʼs book)! Lecture 4! ü Review on atom/ion size! ü Crystal structure (Chap 4 of Nesseʼs book)! 15 C 4+ 42 Si 4+ Size of atoms! Hefferan and O Brien, 2010; Earth Materials Force balance! Crystal structure (Chap. 4)!

More information

03/06/2014. In Glasses, which lack long-range structure completely, this idea works even better!

03/06/2014. In Glasses, which lack long-range structure completely, this idea works even better! Composition Structure Property Correlations In Glasses and Glass Ceramics In Glasses, which lack long-range structure completely, this idea works even better! Hellmut Eckert Instituto da Física Sao Carlos

More information

Atomistics of the Lithiation of Oxidized Silicon. Dynamics Simulations

Atomistics of the Lithiation of Oxidized Silicon. Dynamics Simulations Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2016 Electronic Supplementary Information (ESI) Atomistics of the Lithiation of Oxidized

More information

Pickup velocity of nanoparticles

Pickup velocity of nanoparticles Engineering Conferences International ECI Digital Archives Fluidization XV Proceedings 5-23-2016 Pickup velocity of nanoparticles Jia Wei Chew Singapore Membrane Technology Center, Nanyang Environment

More information

Fabrication Technology, Part I

Fabrication Technology, Part I EEL5225: Principles of MEMS Transducers (Fall 2004) Fabrication Technology, Part I Agenda: Microfabrication Overview Basic semiconductor devices Materials Key processes Oxidation Thin-film Deposition Reading:

More information

Bonding in Solids. What is the chemical bonding? Bond types: Ionic (NaCl vs. TiC?) Covalent Van der Waals Metallic

Bonding in Solids. What is the chemical bonding? Bond types: Ionic (NaCl vs. TiC?) Covalent Van der Waals Metallic Bonding in Solids What is the chemical bonding? Bond types: Ionic (NaCl vs. TiC?) Covalent Van der Waals Metallic 1 Ions and Ionic Radii LiCl 2 Ions (a) Ions are essentially spherical. (b) Ions may be

More information

Chapter 12: Structures & Properties of Ceramics

Chapter 12: Structures & Properties of Ceramics Chapter 12: Structures & Properties of Ceramics ISSUES TO ADDRESS... Bonding and structure of ceramic materials as compared with metals Chapter 12-1 Atomic Bonding in Ceramics Bonding: -- Can be ionic

More information

Segregation of equal-sized particles of different densities in a vertically vibrated fluidized bed

Segregation of equal-sized particles of different densities in a vertically vibrated fluidized bed Engineering Conferences International ECI Digital Archives Fluidization XV Proceedings 5-26-2016 Segregation of equal-sized particles of different densities in a vertically vibrated fluidized bed E. Cano-Pleite

More information

O and Si make up % of all atoms available to make minerals in the Earth's crust.

O and Si make up % of all atoms available to make minerals in the Earth's crust. 7. Minerals III (p. 87-97) Mineral Families O and Si make up % of all atoms available to make minerals in the Earth's crust. Minerals in which cations combine with O 2- anions are called. If Si gets added,

More information

Surface atoms/molecules of a material act as an interface to its surrounding environment;

Surface atoms/molecules of a material act as an interface to its surrounding environment; 1 Chapter 1 Thesis Overview Surface atoms/molecules of a material act as an interface to its surrounding environment; their properties are often complicated by external adsorbates/species on the surface

More information

New Quantum Transport Results in Type-II InAs/GaSb Quantum Wells

New Quantum Transport Results in Type-II InAs/GaSb Quantum Wells New Quantum Transport Results in Type-II InAs/GaSb Quantum Wells Wei Pan Sandia National Laboratories Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation,

More information

Chapter 10. Liquids and Solids

Chapter 10. Liquids and Solids Chapter 10 Liquids and Solids Chapter 10 Table of Contents 10.1 Intermolecular Forces 10.2 The Liquid State 10.3 An Introduction to Structures and Types of Solids 10.4 Structure and Bonding in Metals 10.5

More information

Ionic Bonding - Electrostatic Interactions and Polarization

Ionic Bonding - Electrostatic Interactions and Polarization Ionic Bonding - Electrostatic Interactions and Polarization Chemistry 754 Solid State Chemistry Dr. Patrick Woodward Lecture #13 Born-Haber Cycle for NaCl It is energetically unfavorable for Na metal and

More information

CFD-DEM simulation of nanoparticle agglomerates fluidization with a micro- jet

CFD-DEM simulation of nanoparticle agglomerates fluidization with a micro- jet Engineering Conferences International ECI Digital Archives Fluidization XV Proceedings 5-26-2016 CFD-DEM simulation of nanoparticle agglomerates fluidization with a micro- jet Daoyin Liu Key Laboratory

More information

Advanced Vitreous State - Physical Properties of Glass

Advanced Vitreous State - Physical Properties of Glass Advanced Vitreous State - Physical Properties of Glass Lecture 25: Charge Conduction Properties of Glass: Steve W. Martin Ionic Conduction in Glass - Part 1 Relationship to Glass Structure and Composition

More information

Moulding and Casting Methods 2. Greensand system

Moulding and Casting Methods 2. Greensand system MME 345, Lecture 22 Moulding and Casting Methods 2. Greensand system Ref: [1] Heine, Loper & Rosenthal, Principles of Metal Casting, McGraw-Hill, 1976 [2] Beeley, Foundry Technology, Butterworth-Heinemann,

More information

A comparative study of no-time-counter and majorant collision frequency numerical schemes in DSMC

A comparative study of no-time-counter and majorant collision frequency numerical schemes in DSMC Purdue University Purdue e-pubs School of Aeronautics and Astronautics Faculty Publications School of Aeronautics and Astronautics 2012 A comparative study of no-time-counter and majorant collision frequency

More information

A lattice dynamical investigation of zircon (ZrSiOJ has been carried out to obtain a

A lattice dynamical investigation of zircon (ZrSiOJ has been carried out to obtain a r. -.*. Version Date: 7/14/97 Inelastic Neutron Scattering From Zircon, J. C. Nipko and C.-K.Loong Argonne National Laboratory, Argonne, IL 60439, U.S.A. Abstract A lattice dynamical investigation of zircon

More information

Semester Length Glass Courses and Glass Schools

Semester Length Glass Courses and Glass Schools Lehigh University Lehigh Preserve US-Japan Winter School Semester Length Glass Courses and Glass Schools Winter 1-1-2008 Special lecture, Part 1: Nature-guided nanotechnology for chemical tectonics of

More information

What happens when substances freeze into solids? Less thermal energy available Less motion of the molecules More ordered spatial properties

What happens when substances freeze into solids? Less thermal energy available Less motion of the molecules More ordered spatial properties Chapter #16 Liquids and Solids 16.1) Intermolecular Forces 16.2) The Liquid State 16.3) An Introduction to Structures and Types of Solids 16.4) Structure and Bonding of Metals 16.5) Carbon and Silicon:

More information

Properties of Compounds

Properties of Compounds Chapter 6. Properties of Compounds Comparing properties of elements and compounds Compounds are formed when elements combine together in fixed proportions. The compound formed will often have properties

More information

6. Computational Design of Energy-related Materials

6. Computational Design of Energy-related Materials 6. Computational Design of Energy-related Materials Contents 6.1 Atomistic Simulation Methods for Energy Materials 6.2 ab initio design of photovoltaic materials 6.3 Solid Ion Conductors for Fuel Cells

More information

Mechanical Shock Testing for LIGA Materials Characterization

Mechanical Shock Testing for LIGA Materials Characterization Mechanical Shock Testing for LIGA Materials Characterization Vesta I. Bateman Alfredo M. Morales Principal Member of Technical Staff Sandia National Laboratories* P.O. Box 58, MS553 Albuquerque, NM 87185-553

More information

Atomic Structure & Interatomic Bonding

Atomic Structure & Interatomic Bonding Atomic Structure & Interatomic Bonding Chapter Outline Review of Atomic Structure Atomic Bonding Atomic Structure Atoms are the smallest structural units of all solids, liquids & gases. Atom: The smallest

More information

GLASS Asst. Lect. Shireen Hasan

GLASS Asst. Lect. Shireen Hasan Collage of Engineering Materials Department Third Class Lecture (13) GLASS Asst. Lect. Shireen Hasan 6-3 transport properties: The transport property of glasses is controlled by the diffusion, or transport

More information

The Periodic Table and Chemical Reactivity

The Periodic Table and Chemical Reactivity The and Chemical Reactivity Noble gases Less electronegative elements More electronegative elements Then what is electronegativity? The tendency of an atom to attract an electron (or electron density)

More information

STRUCTURAL BEHAVIOUR OF NIOBIUM PHOSPHATE VITROCERAMICS IN SIMULATED BODY FLUID

STRUCTURAL BEHAVIOUR OF NIOBIUM PHOSPHATE VITROCERAMICS IN SIMULATED BODY FLUID Journal of Optoelectronics and Advanced Materials Vol. 7, No. 6, December 2005, p. 2839-2843 STRUCTURAL BEHAVIOUR OF NIOBIUM PHOSPHATE VITROCERAMICS IN SIMULATED BODY FLUID S. Simon *, V. R. F. Turcu,

More information

EVALUATION OF A.C. CONDUCTIVITY FOR LEAD SILICATE GLASS FROM DIELECTRIC MEASUREMENTS

EVALUATION OF A.C. CONDUCTIVITY FOR LEAD SILICATE GLASS FROM DIELECTRIC MEASUREMENTS Journal of Electron Devices, Vol. 12, 2012, pp. 750-755 JED [ISSN: 1682-3427 ] EVALUATION OF A.C. CONDUCTIVITY FOR LEAD SILICATE GLASS FROM DIELECTRIC MEASUREMENTS D.K. Mahde, B.T.Chiad, Ghuson H.Mohamed

More information

Chemistry 1000 Lecture 22: Group 14 and Boron. Marc R. Roussel

Chemistry 1000 Lecture 22: Group 14 and Boron. Marc R. Roussel Chemistry 1000 Lecture 22: Group 14 and Boron Marc R. Roussel Group 14 In this group again, we see a full range of nonmetallic to metallic behavior: C is a nonmetal. Si and Ge are metalloids. Sn and Pb

More information

Web Course Physical Properties of Glass. Range Behavior

Web Course Physical Properties of Glass. Range Behavior Web Course Physical Properties of Glass Glass Transformation- Range Behavior Richard K. Brow Missouri University of Science & Technology Department of Materials Science & Engineering Glass Transformation-1

More information

Thermal analog to AFM force-displacement measurements for nanoscale interfacial contact resistance

Thermal analog to AFM force-displacement measurements for nanoscale interfacial contact resistance Brigham Young University BYU ScholarsArchive All Faculty Publications 2010 Thermal analog to AFM force-displacement measurements for nanoscale interfacial contact resistance Brian D. Iverson Brigham Young

More information

Earth Materials I Crystal Structures

Earth Materials I Crystal Structures Earth Materials I Crystal Structures Isotopes same atomic number, different numbers of neutrons, different atomic mass. Ta ble 1-1. Su mmar y of quantu m num bers Name Symbol Values Principal n 1, 2,

More information

FEEDBACK CONTROL OF GROWTH RATE AND SURFACE ROUGHNESS IN THIN FILM GROWTH. Yiming Lou and Panagiotis D. Christofides

FEEDBACK CONTROL OF GROWTH RATE AND SURFACE ROUGHNESS IN THIN FILM GROWTH. Yiming Lou and Panagiotis D. Christofides FEEDBACK CONTROL OF GROWTH RATE AND SURFACE ROUGHNESS IN THIN FILM GROWTH Yiming Lou and Panagiotis D. Christofides Department of Chemical Engineering University of California, Los Angeles IEEE 2003 Conference

More information

THE PERIODIC TABLE. Dr Marius K Mutorwa

THE PERIODIC TABLE. Dr Marius K Mutorwa THE PERIODIC TABLE Dr Marius K Mutorwa mmutorwa@polytechnic.edu.na COURSE CONTENT 1. History of the atom 2. Sub-atomic Particles protons, electrons and neutrons 3. Atomic number and Mass number 4. Isotopes

More information

Atomistic Modelling of Oil Shale Kerogens and Asphaltenes

Atomistic Modelling of Oil Shale Kerogens and Asphaltenes Atomistic Modelling of Oil Shale Kerogens and Asphaltenes Julio Facelli*, Anita Orendt, Ian Pimienta, Shyam Badu, Ronald Pugmire 31st Oil Shale Symposium October 17-21, 2011 This work has been partially

More information