Cold Work, Recovery, Recrystallization and Grain Growth
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Using Grain Boundary Irregularity to Quantify Dynamic Recrystallization in Ice
Acta Materialia 209 (2021) 116810 Contents lists available at ScienceDirect Acta Materialia journal homepage: www.elsevier.com/locate/actamat Using grain boundary irregularity to quantify dynamic recrystallization in ice ∗ Sheng Fan a, , David J. Prior a, Andrew J. Cross b,c, David L. Goldsby b, Travis F. Hager b, Marianne Negrini a, Chao Qi d a Department of Geology, University of Otago, Dunedin, New Zealand b Department of Earth and Environmental Science, University of Pennsylvania, Philadelphia, PA, United States c Department of Geology and Geophysics, Woods Hole Oceanographic Institution, Woods Hole, MA, United States d Institute of Geology and Geophysics, Chinese Academy of Sciences, Beijing, China a r t i c l e i n f o a b s t r a c t Article history: Dynamic recrystallization is an important mechanical weakening mechanism during the deformation of Received 24 December 2020 ice, yet we currently lack robust quantitative tools for identifying recrystallized grains in the “migration” Revised 7 March 2021 recrystallization regime that dominates ice deformation at temperatures close to the ice melting point. Accepted 10 March 2021 Here, we propose grain boundary irregularity as a quantitative means for discriminating between recrys- Available online 15 March 2021 tallized (high sphericity, low irregularity) and remnant (low sphericity, high irregularity) grains. To this Keywords: end, we analysed cryogenic electron backscatter diffraction (cryo-EBSD) data of deformed polycrystalline High-temperature deformation ice, to quantify dynamic recrystallization using grain boundary irregularity statistics. Grain boundary ir- Grain boundary irregularity regularity has an inverse relationship with a sphericity parameter, , defined as the ratio of grain area Dynamic recrystallization and grain perimeter, divided by grain radius in 2-D so that the measurement is grain size independent. -
Grain Growth During Spark Plasma and Flash Sintering of Ceramic Nanoparticles: a Review Rachman Chaim, Geoffroy Chevallier, Alicia Weibel, Claude Estournes
Grain growth during spark plasma and flash sintering of ceramic nanoparticles: a review Rachman Chaim, Geoffroy Chevallier, Alicia Weibel, Claude Estournes To cite this version: Rachman Chaim, Geoffroy Chevallier, Alicia Weibel, Claude Estournes. Grain growth during spark plasma and flash sintering of ceramic nanoparticles: a review. Journal of Materials Science, Springer Verlag, 2018, vol. 53 (n° 5), pp. 3087-3105. 10.1007/s10853-017-1761-7. hal-01682331 HAL Id: hal-01682331 https://hal.archives-ouvertes.fr/hal-01682331 Submitted on 12 Jan 2018 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Open Archive TOULOUSE Archive Ouverte (OATAO) OATAO is an open access repository that collects the work of Toulouse researchers and makes it freely available over the web where possible. This is an author-deposited version published in : http://oatao.univ-toulouse.fr/ Eprints ID : 19431 To link to this article : DOI:10.1007/s10853-017-1761-7 URL : http://dx.doi.org/10.1007/s10853-017-1761-7 To cite this version : Chaim, Rachman and Chevallier, Geoffroy and Weibel, Alicia and Estournes, Claude Grain growth during spark plasma and flash sintering of ceramic nanoparticles: a review. -
A Study on Physical Properties of Mortar Mixed with Fly-Ash As Functions of Mill Types and Milling Times
Journal of the Korean Ceramic Society http://dx.doi.org/10.4191/kcers.2016.53.4.435 Vol. 53, No. 4, pp. 435~443, 2016. Communication A Study on Physical Properties of Mortar Mixed with Fly-ash as Functions of Mill Types and Milling Times Sung Kwan Seo*,**, Yong Sik Chu*,†, Kwang Bo Shim**, and Jae Hyun Jeong* *Energy & Environmental Division, Korea Institute of Ceramic Engineering and Technology, Jinju 52851, Korea1) **Division of Materials Science and Engineering, Hanyang University, Seoul 04763, Korea2) (Received January 27, 2016; Revised May 9, July 4, 2016; Accepted July 7, 2016) ABSTRACT Coal ash, a material generated from coal-fired power plants, can be classified as fly ash and bottom ash. The amount of domes- tic fly ash generation is almost 6.84 million tons per year, while the amount of bottom ash generation is 1.51 million tons. The fly ash is commonly used as a concrete admixture and a subsidiary raw material in cement fabrication process. And some amount of bottom ash is used as a material for embankment and block. However, the recyclable amount of the ash is limited since it could cause deterioration of physical properties. In Korea, the ashes are simply mixed and used as a replacement material for cement. In this study, an attempt was made to mechanically activate the ash by grinding process in order to increase recycling rates of the fly ash. Activated fly ash was prepared by controlling the mill types and the milling times and characteristics of the mortar containing the activated fly ash was analyzed. -
Emission of Dislocations from Grain Boundaries and Its Role in Nanomaterials
crystals Review Emission of Dislocations from Grain Boundaries and Its Role in Nanomaterials James C. M. Li 1,*, C. R. Feng 2 and Bhakta B. Rath 2 1 Department of Mechanical Engineering, University of Rochester, Rochester, NY 14627, USA 2 U.S. Naval Research Laboratory, 4555 Overlook Ave SW, Washington, DC 20375, USA; [email protected] (C.R.F.); [email protected] (B.B.R.) * Correspondence: [email protected] Abstract: The Frank-Read model, as a way of generating dislocations in metals and alloys, is widely accepted. In the early 1960s, Li proposed an alternate mechanism. Namely, grain boundary sources for dislocations, with the aim of providing a different model for the Hall-Petch relation without the need of dislocation pile-ups at grain boundaries, or Frank-Read sources inside the grain. This article provides a review of his model, and supporting evidence for grain boundaries or interfacial sources of dislocations, including direct observations using transmission electron microscopy. The Li model has acquired new interest with the recent development of nanomaterial and multilayers. It is now known that nanocrystalline metals/alloys show a behavior different from conventional polycrystalline materials. The role of grain boundary sources in nanomaterials is reviewed briefly. Keywords: dislocation emission; grain boundaries; nanomaterials; Hall-Petch relation; metals and alloys 1. Introduction To explain the properties of crystalline aggregates, such as crystal plasticity, Taylor [1,2] provided a theoretical construct of line defects in the atomic scale of the crystal lattice. Citation: Li, J.C.M.; Feng, C.R.; With the use of the electron microscope, the sample presence of dislocations validated Rath, B.B. -
ROLLING of METAL (Auxiliary Operations Used in Connection With
CPC - B21B - 2017.08 B21B ROLLING OF METAL (auxiliary operations used in connection with metal- working operations covered in B21, see B21C; bending by rolling B21D; manufacture of particular objects, e.g. screws, wheels, rings, barrels, balls, by rolling B21H; pressure welding by means of a rolling mill B23K 20/04) Definition statement This place covers: Methods and devices for rolling of metal. Rolling is a metal forming process in which metal is passed through a pair of rotating rolls for plastic deformation of the metall. Rolling is classified according to the temperature of the metal rolled. If the temperature of the metal is above its recrystallization temperature, then the process is termed as hot rolling. If the temperature of the metal is below its recrystallization temperature, the process is termed as cold rolling. A rolling mill is a machine for plastic deformation of metal between rotating rolls. In a broader sense, a rolling mill is an automatic system or line of machines that performs both rolling and auxiliary operations: transport of the original billet from the stock to the heating furnaces and the mill rolls, transfer of the rolled material from one groove to another, turning, transport of the metal after rolling, cutting into sections, marking or stamping, trimming, packing, and conveyance to the stock of finished product. This subclass includes the following main groups: Rolling of metal in general: • Methods or devices in general B21B 1/00, B21B 11/00 - B21B 13/00 • Control B21B 37/00 • Measuring B21B 38/00 • Operation B21B 35/00, B21B 39/00, B21B 41/00 • Details of rolling mills B21B 27/00, B21B 29/00, B21B 31/00 • Maintenance of rolling rolls B21B 28/00 • Safety devices B21B 33/00 • Cooling beds and accessories B21B 43/00 Rolling of special formats: • tube rolling B21B 17/00, B21B 19/00, B21B 23/00 1 B21B (continued) CPC - B21B - 2017.08 • accessories for tube rolling B21B 25/00 • Extending closed shapes of metal bands B21B 5/00 Rolling of special alloys: B21B 3/00 Rolling of metal under special conditions (e.g. -
Multidisciplinary Design Project Engineering Dictionary Version 0.0.2
Multidisciplinary Design Project Engineering Dictionary Version 0.0.2 February 15, 2006 . DRAFT Cambridge-MIT Institute Multidisciplinary Design Project This Dictionary/Glossary of Engineering terms has been compiled to compliment the work developed as part of the Multi-disciplinary Design Project (MDP), which is a programme to develop teaching material and kits to aid the running of mechtronics projects in Universities and Schools. The project is being carried out with support from the Cambridge-MIT Institute undergraduate teaching programe. For more information about the project please visit the MDP website at http://www-mdp.eng.cam.ac.uk or contact Dr. Peter Long Prof. Alex Slocum Cambridge University Engineering Department Massachusetts Institute of Technology Trumpington Street, 77 Massachusetts Ave. Cambridge. Cambridge MA 02139-4307 CB2 1PZ. USA e-mail: [email protected] e-mail: [email protected] tel: +44 (0) 1223 332779 tel: +1 617 253 0012 For information about the CMI initiative please see Cambridge-MIT Institute website :- http://www.cambridge-mit.org CMI CMI, University of Cambridge Massachusetts Institute of Technology 10 Miller’s Yard, 77 Massachusetts Ave. Mill Lane, Cambridge MA 02139-4307 Cambridge. CB2 1RQ. USA tel: +44 (0) 1223 327207 tel. +1 617 253 7732 fax: +44 (0) 1223 765891 fax. +1 617 258 8539 . DRAFT 2 CMI-MDP Programme 1 Introduction This dictionary/glossary has not been developed as a definative work but as a useful reference book for engi- neering students to search when looking for the meaning of a word/phrase. It has been compiled from a number of existing glossaries together with a number of local additions. -
Strengthening Mechan
9-17-2014 Wednesday, September 17, 2014 6:50 AM Strengthening mechanisms •stretching is due to plastic deformation •plastic deformation is due to Motion of dislocations • to strengthen Materials, make it harder for dislocations to move. ENGR45-strengthening mech Page 1 Example: Calculate 0 and Ky and estimate YS of a polyxrystalline brass with ASTM number 8 From interactive graph we find: Solve: Use M=1 and n=8, you get N=1.28x106 •It means •So ENGR45-strengthening mech Page 2 ENGR45-strengthening mech Page 3 3)Work hardening, strain hardening, Cold working, more later Effect of cold work on tensile stress-strain curve for low-carbon steel bars. Pasted from <http://www.daldermaterialsconsulting.com/html/materials-engineering.html> ENGR45-strengthening mech Page 4 4)ppt hardening (or Age hardening) more Later. ENGR45-strengthening mech Page 5 Dislocations create Plastic deformation by "slip" "SLIP" occurs as shear in slip system consisting of SLIP PLANE and SLIP DIRECTION. Both SLIP PLANE and SLIP DIRECTION are closed pack. In BCC, SLIP PLANE is (110) and SLIP DIRECTION is [111] In FCC, SLIP PLANE is (111) and SLIP DIRECTION is [110] (6planes)*(2 directions) =12 systems ENGR45-strengthening mech Page 6 Slip system in FCC, (111) and [110) (4 planes)*(3 directions) =12 systems ENGR45-strengthening mech Page 7 Schmid's factor ENGR45-strengthening mech Page 8 ENGR45-strengthening mech Page 9 More on Cold working, Strain Hardening, work hardening. These are all examples of C.W: Rolling Bending Shearing Swaging Angle Tube drawing Slitting Extrusion -
Copper Alloys
THE COPPER ADVANTAGE A Guide to Working With Copper and Copper Alloys www.antimicrobialcopper.com CONTENTS I. Introduction ............................. 3 PREFACE Conductivity .....................................4 Strength ..........................................4 The information in this guide includes an overview of the well- Formability ......................................4 known physical, mechanical and chemical properties of copper, Joining ...........................................4 as well as more recent scientific findings that show copper has Corrosion ........................................4 an intrinsic antimicrobial property. Working and finishing Copper is Antimicrobial ....................... 4 techniques, alloy families, coloration and other attributes are addressed, illustrating that copper and its alloys are so Color ..............................................5 adaptable that they can be used in a multitude of applications Copper Alloy Families .......................... 5 in almost every industry, from door handles to electrical circuitry to heat exchangers. II. Physical Properties ..................... 8 Copper’s malleability, machinability and conductivity have Properties ....................................... 8 made it a longtime favorite metal of manufacturers and Electrical & Thermal Conductivity ........... 8 engineers, but it is its antimicrobial property that will extend that popularity into the future. This guide describes that property and illustrates how it can benefit everything from III. Mechanical -
Atomic Resolution Electron Tomography for 3D Imaging of Dislocations in Nanoparticles
Atomic Resolution Electron Tomography for 3D Imaging of Dislocations in Nanoparticles Chien-Chun Chen1,2, Chun Zhu1,2, Edward R. White1,2, Chin-Yi Chiu2,3, M. C. Scott1,2, B. C. Regan1,2, Laurence D. Marks4, Yu Huang2,3 and Jianwei Miao1 1Department of Physics and Astronomy, University of California, Los Angeles, CA 90095, USA. 2California NanoSystems Institute, University of California, Los Angeles, CA 90095, USA. 3Department of Materials Science and Engineering, University of California, Los Angeles, CA 90095, USA. 4Department of Materials Science and Engineering, Northwestern University, Evanston, IL 60201, USA. Dislocations and their interactions strongly influence many of the properties of materials, ranging from the strength of metals and alloys to the efficiency of light-emitting diodes and laser diodes. Although various experimental methods have been used to image dislocations in materials since 1956, a 3D technique for visualizing dislocations at atomic resolution has not previously been demonstrated. Here we report the development of atomic resolution electron tomography and achieve 3D imaging of dislocation core structures of a Pt nanoparticle at atomic resolution. Compared to conventional electron tomography, our atomic resolution imaging method incorporates three novel developments. First, the conventional alignment approach used in electron tomography either relies on fiducial markers or is based on the cross-correlation between neighboring projections. To our knowledge, neither of these alignment approaches can achieve atomic level precision. To overcome this limitation, we have developed a method based on the center of mass (CM), which is able to align the projections of a tilt series at atomic level accuracy. Second, we have implemented a data acquisition and tomographic reconstruction method, termed equally sloped tomography (EST). -
Properties of the Phase Components of the Modified Cement System
TEKA. COMMISSION OF MOTORIZATION AND ENERGETICS IN AGRICULTURE – 2013, Vol. 13, No.4, 218-224 Properties of the phase components of the modified cement system Dmytro Rudenko Volodymyr Dahl East-Ukrainian National University, Molodizhny bl., 20ɚ, Lugansk, 91034, Ukraine, e-mail: [email protected] Received September 18.2013: accepted October 09.2013 S u m m a r y : The article presents the results of the properties. The simplest way of intensification study of the influence of modification on the clinker of hydration process and optimization of mono minerals structure formation. A research of synthesized and modified mineral systems resistance to cement systems structure formation is a usage the weathering (carbonation, varying conditions), as of polyfunctional admixtures [5, 11, 16, 19, well as to the aggressive solutions exposure was 23]. Such additives, intensifying hydration conducted. process, having an effect on the hydration K e y w o r d s : cement system, modification, mono products morphology and their structure minerals, resistance. formation process, can’t be composed of one component [15, 27, 28, 30]. Obviously, such INTRODUCTION additives must form a complex with polyfunctional properties. At the same time, There are many ways of purposeful organic plasticizers, widely used at building control of structure formation of the concrete industry enterprises, require an addition with mixtures’ cement systems at different stages of special mineral components, chemically hardening [1, 3, 6]. The most rational way is a interacting with clinker minerals. Thus, it’s structure adjustment through the introduction necessary to choose a complex composition of modifiers. Modification of cement systems modifier with polyfunctional effect on the by various chemically-active components structuring cement system. -
Defects in Semiconductor Crystals Lecture 6 Oct
ECE236A Semiconductor Heterostructure Materials Defects in Semiconductor Crystals Lecture 6 Oct. 10-14, 2019 • Stacking sequence in simple crystals. • Stacking faults (intrinsic, extrinsic) • Twin boundaries • Dislocations and Burgers Vectors • Shockely and Franck partial dislocations. • Thompson Tetrahedron. • Dislocations in Hexagonal, Covalent and polar/nonpolar epitaxial crystals. • Polar Materials on non-Polar Substrates. Ref.: Introduction to Dislocations, D. Hull and D.J. Bacon, 4th ed. Elsevier, 2001. 1 Stacking Sequence (1) • Stacking sequence: To describe the arrangement of lattice sites within a crystal structure, we refer to the order or sequence of the atom layers in the ‘stack’ as ‘stacking sequence’. Simple cubic structure: Lattice sites are identical when Lattice sites are displaced by a/21/2 projected normal to the (100) plane in the [-110] direction à AAA… stacking à ABABAB… stacking (100) layers (110) layers Body Centered Cubic: (110) layers 2 Stacking Sequence (2) Face centered cubic structure: Arrangement of atoms in (111) plane Stacking sequence (111) plane in one lattice Close packed (111) plane (110) à ABABAB… (111) à ABCABCABC… Si C A B C A C B B A A 3 J.W. Morris, UC Berkeley DayeH, SST 25, 02424 2010. Yoo & DayeH, APL, 2013. Stacking Sequence (3) Hexagonal crystal structure: cubic hexagonal 4 http://www.hardmaterials.de/html/diamonds__ionsdaleite.html Stacking Faults • Are planar defects where the regular sequence in the crystal has been interrupted. • Cannot occur with ABAB stacking but can occur in ABC stacking because layers in A have alternative position in close packed layers to rest in either A or B positions. • Two types: 1 less A layer – Intrinsic Si C B C B A B C B A – Extrinsic http://www.ece.umn.edu/groups/nsfret/TEMpics.html 1 additional B layer Fault energy: 1 – 1000 mJ/m2 • Usually occur with composition change, high doping levels, and non-optimal growth conditions. -
Dislocation Structure Evolution During Plastic Deformation of Low-Carbon Steel
IEJME — MATHEMATICS EDUCATION 2016, VOL. 11, NO. 6, 1563-1576 OPEN ACCESS Dislocation Structure Evolution during Plastic Deformation of Low-Carbon Steel Georgii I. Raaba, Yurii M. Podrezovb, Mykola I. Danylenkob, Katerina M. Borysovskab, Gennady N. Aleshina c and Lenar N. Shafigullin a Ufa State Aviation Technical University (USATU), Ufa, RUSSIA; bFrantsevich Institute for Problems of Materials Science, Kiev, UKRAINE; cNaberezhnye Chelny Institute is the first branch of Kazan Federal University, Naberezhnye Chelny, RUSSIA. ABSTRACT In this paper, the regularities of structure formation in low-alloyed carbon steels are analyzed. They coincide to a large extent with the general views on the effect of strain degree on the evolution of deformation structure. In ferrite grains, not only the qualitative picture of changes, well known for Armco iron, is repeated, but also the quantitative values of strain corresponding to a change in the structural state are repeated as well. When investigating samples of a ferritic- pearlitic steel, it is found that structure formation in pearlite essentially lags behind structural changes in ferrite grains, and this delay is observed at all stages of deformation. An important feature of structure formation in pearlite is crack nucleation in cementite, accompanied by dislocation pile-up in the ferrite interlayers of pearlite. Using the method of dislocation dynamics, the relationship between structural transformations and the parameters of strain hardening is analyzed. It is demonstrated that the proposed method of computer analysis reflects well the processes taking place in a material during plastic deformation. The character of the theoretical curve of strain hardening is determined by the dislocation structure that forms in a material at various stages of deformation.