Graphite Materials for the U.S
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The Era of Carbon Allotropes Andreas Hirsch
commentary The era of carbon allotropes Andreas Hirsch Twenty-five years on from the discovery of 60C , the outstanding properties and potential applications of the synthetic carbon allotropes — fullerenes, nanotubes and graphene — overwhelmingly illustrate their unique scientific and technological importance. arbon is the element in the periodic consist of extended networks of sp3- and 1985, with the advent of fullerenes (Fig. 1), table that provides the basis for life sp2 -hybridized carbon atoms, respectively. which were observed for the first time by Con Earth. It is also important for Both forms show unique physical properties Kroto et al.3. This serendipitous discovery many technological applications, ranging such as hardness, thermal conductivity, marked the beginning of an era of synthetic from drugs to synthetic materials. This lubrication behaviour or electrical carbon allotropes. Now, as we celebrate role is a consequence of carbon’s ability conductivity. Conceptually, many other buckminsterfullerene’s 25th birthday, it is to bind to itself and to nearly all elements ways to construct carbon allotropes are also the time to reflect on a growing family in almost limitless variety. The resulting possible by altering the periodic binding of synthetic carbon allotropes, which structural diversity of organic compounds motif in networks consisting of sp3-, sp2- includes the synthesis of carbon nanotubes and molecules is accompanied by a broad and sp-hybridized carbon atoms1,2. As a in 19914 and the rediscovery of graphene range of -
Chemistry with Graphene and Graphene Oxide - Challenges for Synthetic Chemists Siegfried Eigler* and Andreas Hirsch*
Chemistry with Graphene and Graphene Oxide - Challenges for Synthetic Chemists Siegfried Eigler* and Andreas Hirsch* Dr. Siegfried Eigler*, Prof. Dr. Andreas Hirsch* Department of Chemistry and Pharmacy and Institute of Advanced Materials and Processes (ZMP) Henkestrasse 42, 91054 Erlangen and Dr.-Mack Strasse 81, 90762 Fürth (Germany) Fax: (+49) 911-6507865015 E-mail: [email protected]; [email protected] The chemical production of graphene as well as its controlled wet- chemical modification is a challenge for synthetic chemists and the characterization of reaction products requires sophisticated analytic methods. In this review we first describe the structure of graphene and graphene oxide. We then outline the most important synthetic methods which are used for the production of these carbon based nanomaterials. We summarize the state-of-the-art for their chemical functionalization by non-covalent and covalent approaches. We put special emphasis on the differentiation of the terms graphite, graphene, graphite oxide and graphene oxide. An improved fundamental knowledge about the structure and the chemical properties of graphene and graphene oxide is an important prerequisite for the development of practical applications. 1. Introduction: Graphene and Graphene Oxide – Opportunities and Challenges for Synthetic Chemists Research into graphene and graphene oxide (GO) represents an emerging field of interdisciplinary science spanning a variety of disciplines including chemistry, physics, materials science, device fabrication and -
Coal Characteristics
CCTR Indiana Center for Coal Technology Research COAL CHARACTERISTICS CCTR Basic Facts File # 8 Brian H. Bowen, Marty W. Irwin The Energy Center at Discovery Park Purdue University CCTR, Potter Center, 500 Central Drive West Lafayette, IN 47907-2022 http://www.purdue.edu/dp/energy/CCTR/ Email: [email protected] October 2008 1 Indiana Center for Coal Technology Research CCTR COAL FORMATION As geological processes apply pressure to peat over time, it is transformed successively into different types of coal Source: Kentucky Geological Survey http://images.google.com/imgres?imgurl=http://www.uky.edu/KGS/coal/images/peatcoal.gif&imgrefurl=http://www.uky.edu/KGS/coal/coalform.htm&h=354&w=579&sz= 20&hl=en&start=5&um=1&tbnid=NavOy9_5HD07pM:&tbnh=82&tbnw=134&prev=/images%3Fq%3Dcoal%2Bphotos%26svnum%3D10%26um%3D1%26hl%3Den%26sa%3DX 2 Indiana Center for Coal Technology Research CCTR COAL ANALYSIS Elemental analysis of coal gives empirical formulas such as: C137H97O9NS for Bituminous Coal C240H90O4NS for high-grade Anthracite Coal is divided into 4 ranks: (1) Anthracite (2) Bituminous (3) Sub-bituminous (4) Lignite Source: http://cc.msnscache.com/cache.aspx?q=4929705428518&lang=en-US&mkt=en-US&FORM=CVRE8 3 Indiana Center for Coal Technology Research CCTR BITUMINOUS COAL Bituminous Coal: Great pressure results in the creation of bituminous, or “soft” coal. This is the type most commonly used for electric power generation in the U.S. It has a higher heating value than either lignite or sub-bituminous, but less than that of anthracite. Bituminous coal -
Molten Salt Chemistry Workshop
The cover depicts the chemical and physical complexity of the various species and interfaces within a molten salt reactor. To advance new approaches to molten salt technology development, it is necessary to understand and predict the chemical and physical properties of molten salts under extreme environments; understand their ability to coordinate fissile materials, fertile materials, and fission products; and understand their interfacial reactions with the reactor materials. Modern x-ray and neutron scattering tools and spectroscopy and electrochemical methods can be coupled with advanced computational modeling tools using high performance computing to provide new insights and predictive understanding of the structure, dynamics, and properties of molten salts over a broad range of length and time scales needed for phenomenological understanding. The actual image is a snapshot from an ab initio molecular dynamics simulation of graphene- organic electrolyte interactions. Image courtesy of Bobby G. Sumpter of ORNL. Molten Salt Chemistry Workshop Report for the US Department of Energy, Office of Nuclear Energy Workshop Molten Salt Chemistry Workshop Technology and Applied R&D Needs for Molten Salt Chemistry April 10–12, 2017 Oak Ridge National Laboratory Co-chairs: David F. Williams, Oak Ridge National Laboratory Phillip F. Britt, Oak Ridge National Laboratory Working Group Co-chairs Working Group 1: Physical Chemistry and Salt Properties Alexa Navrotsky, University of California–Davis Mark Williamson, Argonne National Laboratory Working -
Properties and Characteristics of Graphite
SPECIALTY MATERIALS PROPERTIES AND CHARACTERISTICS OF GRAPHITE For the semiconductor industry May 2013 INTRODUCTION Introduction Table of Contents As Entegris has continued to grow its market share of Introduction .............................................................1 manufactured graphite material and to expand their usage into increasingly complex areas, the need to Structure ..................................................................2 be more technically versed in both Entegris’ POCO® graphite and other manufactured graphite properties Apparent Density .....................................................6 and how they are tested has also grown. It is with this Porosity ....................................................................8 thought in mind that this primer on properties and characteristics of graphite was developed. Hardness ................................................................11 POCO, now owned by Entegris, has been a supplier Compressive Strength .............................................12 to the semiconductor industry for more than 35 years. Products include APCVD wafer carriers, E-Beam cruci- Flexural Strength ...................................................14 bles, heaters (small and large), ion implanter parts, Tensile Strength .....................................................16 LTO injector tubes, MOCVD susceptors, PECVD wafer trays and disk boats, plasma etch electrodes, quartz Modulus of Elasticity .............................................18 replacement parts, sealing -
Graphene: a Peculiar Allotrope of Carbon
Graphene: A Peculiar Allotrope Of Carbon Laxmi Nath Bhattarai Department of Physics, Butwal Multiple Campus Correspondence: [email protected] Abstract Graphene is a two dimensional one atom thick allotrope of Carbon. Electrons in grapheme behave as massless relativistic particles. It is a 2 dimensional nanomaterial with many peculiar properties. In grapheme both integral and fractional quantum Hall effects are observed. Many practical application are seen from use of Graphene material. Keywords: Graphene, allotrope, Quantum Hall effect, nanomaterial. Introduction Graphene is a two dimensional allotropic form of Honey comb structure of Graphene carbon. This was discovered in 2004. Diamond and Graphene is considered as the mother of all graphitic Graphite are three dimensional allotropes of carbon materials because it is the building block of carbon which are known from ancient time. One dimensional materials of all other dimensions (Srinivasan, 2007). carbon nanotubes were discovered in 1991 and Griphite is obtained by the stacking of Graphene zero dimensional Fullerenes were discovered in layers, Diamond can be obtained from Graphene under 1985. Graphene was experimentally extracted from extreme pressure and temperatures. One-dimensional 3-dimensional Graphite by Physisists Andre Geim and carbon nanotubes can be obtained by rolling and Konstantin Novoselov of Manchester University UK Zero–dimensional Fullerenes is obtained by wrapping in 2004. For their remarkable work they were awarded Graphene layers. the Nobel Prize of Physics for the year 2010. Properties Structure The young material Graphene is found to have Graphene is a mono layer of Carbon atoms packed following unique properties: into a honeycomb crystal structure. Graphene sheets 2 are one atom thick 2-dimensional layers of sp – bonded a) It is the thinnest material in the universe and the carbon. -
Nuclear Graphite for High Temperature Reactors
Nuclear Graphite for High temperature Reactors B J Marsden AEA Technology Risley, Warrington Cheshire, WA3 6AT, UK Abstract The cores and reflectors in modem High Temperature Gas Cooled Reactors (HTRs) are constructed from graphite components. There are two main designs; the Pebble Bed design and the Prism design, see Table 1. In both of these designs the graphite not only acts as a moderator, but is also a major structural component that may provide channels for the fuel and coolant gas, channels for control and safety shut off devices and provide thermal and neutron shielding. In addition, graphite components may act as a heat sink or conduction path during reactor trips and transients. During reactor operation, many of the graphite component physical properties are significantly changed by irradiation. These changes lead to the generation of significant internal shrinkage stresses and thermal shut down stresses that could lead to component failure. In addition, if the graphite is irradiated to a very high irradiation dose, irradiation swelling can lead to a rapid reduction in modulus and strength, making the component friable. The irradiation behaviour of graphite is strongly dependent on its virgin microstructure, which is determined by the manufacturing route. Nevertheless, there are available, irradiation data on many obsolete graphites of known microstructures. There is also a well-developed physical understanding of the process of irradiation damage in graphite. This paper proposes a specification for graphite suitable for modem HTRs. HTR Graphite Component Design and Irradiation Environment The details of the HTRs, which have, or are being, been built and operated, are listed in Table 1. -
Mon. Oct 29, 2018 Room1 Plenary Talk 1
Mon. Oct 29, 2018 Plenary Talk The 9th International Conference on Multiscale Materials Modeling Mon. Oct 29, 2018 Room1 Plenary Talk | Plenary Talk [PL1] Plenary Talk 1 Chair: Ju Li(MIT, USA) 10:10 AM - 11:00 AM Room1 [PL1] Plenary Talk 1 ○Christopher A. Schuh (Department of Materials Science and Engineering, MIT, USA) Plenary Talk | Plenary Talk [PL2] Plenary Talk 2 Chair: Alexey Lyulin(Technische Universiteit Eindhoven, The Netherlands) 11:00 AM - 11:50 AM Room1 [PL2] Plenary Talk 2 ○Maenghyo Cho (School of Mechanical and Aerospace Engineering, Seoul National University, Korea) ©The 9th International Conference on Multiscale Materials Modeling Mon. Oct 29, 2018 Symposium The 9th International Conference on Multiscale Materials Modeling Mon. Oct 29, 2018 Sauzay2, Mihai Cosmin Marinica1, Normand Mousseau3 Room1 (1.SRMP-CEA Saclay, France, 2.SRMA-CEA Saclay, France, 3.Département de Physique, Université de Symposium | C. Crystal Plasticity: From Electrons to Dislocation Montréal , Canada) Microstructure [SY-C1] Symposium C-1 Symposium | C. Crystal Plasticity: From Electrons to Dislocation Chair: Emmanuel Clouet(CEA Saclay, SRMP, France) Microstructure 1:30 PM - 3:15 PM Room1 [SY-C2] Symposium C-2 Chair: Stefan Sandfeld(Chair of Micromechanical Materials [SY-C1] Kinetic Monte Carlo model of screw dislocation- Modelling, TU Bergakademie Freiberg, Germany) solute coevolution in W-Re alloys 3:45 PM - 5:30 PM Room1 Yue Zhao1, Lucile Dezerald3, ○Jaime Marian1,2 (1.Dept. [SY-C2] Finite deformation Mesoscale Field Dislocation of Materials Science -
Inhibition of Oxidation in Nuclear Graphite
NEA/NSC/WPFC/DOC(2015)9 Inhibition of oxidation in nuclear graphite Philip L. Winston, James W. Sterbentz and William E. Windes Idaho National Laboratory, United States Abstract Graphite is a fundamental material of high-temperature gas-cooled nuclear reactors, providing both structure and neutron moderation. Its high thermal conductivity, chemical inertness, thermal heat capacity, and high thermal structural stability under normal and off-normal conditions contribute to the inherent safety of these reactor designs. One of the primary safety issues for a high-temperature graphite reactor core is the possibility of rapid oxidation of the carbon structure during an off-normal design basis event where an oxidising atmosphere (air ingress) can be introduced to the hot core. Although the current Generation IV high-temperature reactor designs attempt to mitigate any damage caused by a postualed air ingress event, the use of graphite components that inhibit oxidation is a logical step to increase the safety of these reactors. Recent experimental studies of graphite containing between 5.5 and 7 wt% boron carbide (B4C) indicate that oxidation is dramatically reduced even at prolonged exposures at temperatures up to 900°C. The proposed addition of B4C to graphite components in the nuclear core would necessarily be enriched in B-11 isotope in order to minimise B-10 neutron absorption and graphite swelling. The enriched boron can be added to the graphite during billet fabrication. Experimental oxidation rate results and potential applications for borated graphite in nuclear reactor components will be discussed. Introduction Current Generation IV high-temperature gas-cooled reactors (HTR) are predominately constructed of graphite structural components and graphite fuel elements. -
Investigation of the Stress Induced Properties of Coke During Carbonization
Graduate Theses, Dissertations, and Problem Reports 2007 Investigation of the stress induced properties of coke during carbonization James Joshua Maybury West Virginia University Follow this and additional works at: https://researchrepository.wvu.edu/etd Recommended Citation Maybury, James Joshua, "Investigation of the stress induced properties of coke during carbonization" (2007). Graduate Theses, Dissertations, and Problem Reports. 1959. https://researchrepository.wvu.edu/etd/1959 This Thesis is protected by copyright and/or related rights. It has been brought to you by the The Research Repository @ WVU with permission from the rights-holder(s). You are free to use this Thesis in any way that is permitted by the copyright and related rights legislation that applies to your use. For other uses you must obtain permission from the rights-holder(s) directly, unless additional rights are indicated by a Creative Commons license in the record and/ or on the work itself. This Thesis has been accepted for inclusion in WVU Graduate Theses, Dissertations, and Problem Reports collection by an authorized administrator of The Research Repository @ WVU. For more information, please contact [email protected]. Investigation of the Stress Induced Properties of Coke during Carbonization James Joshua Maybury Thesis submitted to the College of Engineering and Mineral Resources at West Virginia University Master of Science in Mechanical Engineering W. Scott Wayne, Ph.D., Chair Thomas R. Long, Ph.D. Peter G. Stansberry, Ph.D. Alfred H. Stiller, Ph.D. Department of Mechanical and Aerospace Engineering Morgantown, West Virginia 2007 Keywords: Coke, Texture, Anisotropic, Coking, Needle Coke, Pitch Coke, Metallurgical Coke Abstract Investigation of the Stress Induced Properties of Coke during Carbonization James J. -
Surface Analysis of Nuclear Graphite
Keywords Surface analysis Graphite, XPS, 2 of nuclear graphite Auger d-parameter, sp Application Note MO426(1) Further application/technical notes are available online at: www.kratos.com Overview Introduction In this short study we will explore the differences in Graphite is one of the key materials used in the current generation of nuclear reactors in the UK. Since the early days of nuclear fission surface chemistry between two different graphites used graphite has been recognised as an excellent neutron moderator in the nuclear industry. In recent times a wide variety and reflector allowing sustainable controlled fission. of nanostructured carbon forms have been observed in Contaminants in moderator rods are a major problem as they nuclear graphite which vary the graphitic nature of the can act as neutron absorbers. This causes decreased fission and material. The nature of these forms can greatly affect production of unwanted isotopes – a common cause of radioactive waste. The goal of this application is to understand the surface the material’s ability to act as an effective moderator. chemistry of two different graphites: Pile Grade A (PGA) and Here we will discuss the elemental composition of the Gilsocarbon (Gilso). PGA is an early form of nuclear graphite used graphite surface and the extent of graphitic sp2 bonding. in many reactors world-wide, particularly in the UK in the Magnox series. It is derived from a petroleum coke (which is a by-product of the oil refining industry). Gilsocarbon was developed later and is used in the Generation II Advanced Gas-Cooled Reactors. The Gilsonite coke is produced from refining the asphalt. -
Coal As an Abundant Source of Graphene Quantum Dots
ARTICLE Received 8 Jul 2013 | Accepted 14 Nov 2013 | Published 6 Dec 2013 DOI: 10.1038/ncomms3943 Coal as an abundant source of graphene quantum dots Ruquan Ye1,*, Changsheng Xiang1,*, Jian Lin2, Zhiwei Peng1, Kewei Huang1, Zheng Yan1, Nathan P. Cook1, Errol L.G. Samuel1, Chih-Chau Hwang1, Gedeng Ruan1, Gabriel Ceriotti1, Abdul-Rahman O. Raji1, Angel A. Martı´1,3 & James M. Tour1,2,3 Coal is the most abundant and readily combustible energy resource being used worldwide. However, its structural characteristic creates a perception that coal is only useful for pro- ducing energy via burning. Here we report a facile approach to synthesize tunable graphene quantum dots from various types of coal, and establish that the unique coal structure has an advantage over pure sp2-carbon allotropes for producing quantum dots. The crystalline carbon within the coal structure is easier to oxidatively displace than when pure sp2-carbon structures are used, resulting in nanometre-sized graphene quantum dots with amorphous carbon addends on the edges. The synthesized graphene quantum dots, produced in up to 20% isolated yield from coal, are soluble and fluorescent in aqueous solution, providing promise for applications in areas such as bioimaging, biomedicine, photovoltaics and optoelectronics, in addition to being inexpensive additives for structural composites. 1 Department of Chemistry, Rice University, 6100 Main Street, Houston, Texas 77005, USA. 2 Department of Mechanical Engineering and Materials Science, Rice University, 6100 Main Street, Houston, Texas 77005, USA. 3 Smalley Institute for Nanoscale Science and Technology, Rice University, 6100 Main Street, Houston, Texas 77005, USA. * These authors contributed equally to this work.