Development of Microstructure During Sintering and Aluminium Exposure of Titanium Diboride Ceramics
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Quartz Grainsize Evolution During Dynamic Recrystallization Across a Natural Shear Zone Boundary
Journal of Structural Geology 109 (2018) 120–126 Contents lists available at ScienceDirect Journal of Structural Geology journal homepage: www.elsevier.com/locate/jsg Quartz grainsize evolution during dynamic recrystallization across a natural T shear zone boundary ∗ Haoran Xia , John P. Platt Department of Earth Sciences, University of Southern California, Los Angeles, CA 90089-0740, USA ARTICLE INFO ABSTRACT Keywords: Although it is widely accepted that grainsize reduction by dynamic recrystallization can lead to strain locali- Dynamic recrystallization zation, the details of the grainsize evolution during dynamic recrystallization remain unclear. We investigated Bulge the bulge size and grainsizes of quartz at approximately the initiation and the completion stages of bulging Subgrain recrystallization across the upper boundary of a 500 m thick mylonite zone above the Vincent fault in the San Grainsize evolution Gabriel Mountains, southern California. Within uncertainty, the average bulge size of quartz, 4.7 ± 1.5 μm, is Vincent fault the same as the recrystallized grainsize, 4.5 ± 1.5 μm, at the incipient stage of dynamic recrystallization, and also the same within uncertainties as the recrystallized grainsize when dynamic recrystallization is largely complete, 4.7 ± 1.3 μm. These observations indicate that the recrystallized grainsize is controlled by the nu- cleation process and does not change afterwards. It is also consistent with the experimental finding that the quartz recrystallized grainsize paleopiezometer is independent of -
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 Boundary Loops in Graphene
Grain Boundary Loops in Graphene Eric Cockayne,1§ Gregory M. Rutter,2,3 Nathan P. Guisinger,3* Jason N. Crain,3 Phillip N. First,2 and Joseph A. Stroscio3§ 1Ceramics Division, NIST, Gaithersburg, MD 20899 2School of Physics, Georgia Institute of Technology, Atlanta, GA 30332 3Center for Nanoscale Science and Technology, NIST, Gaithersburg, MD 20899 Topological defects can affect the physical properties of graphene in unexpected ways. Harnessing their influence may lead to enhanced control of both material strength and electrical properties. Here we present a new class of topological defects in graphene composed of a rotating sequence of dislocations that close on themselves, forming grain boundary loops that either conserve the number of atoms in the hexagonal lattice or accommodate vacancy/interstitial reconstruction, while leaving no unsatisfied bonds. One grain boundary loop is observed as a “flower” pattern in scanning tunneling microscopy (STM) studies of epitaxial graphene grown on SiC(0001). We show that the flower defect has the lowest energy per dislocation core of any known topological defect in graphene, providing a natural explanation for its growth via the coalescence of mobile dislocations. §Authors to whom correspondence should be addressed:[email protected], [email protected] * Present address: Argonne National Laboratory, Argonne, IL 1 I. Introduction The symmetry of the graphene honeycomb lattice is a key element for determining many of graphene's unique electronic properties. The sub-lattice symmetry of graphene gives rise to its low energy electronic structure, which is characterized by linear energy-momentum dispersion.1 The spinor-like eigenstates of graphene lead to one of its celebrated properties, reduced backscattering (i.e., high carrier mobility), which results from pseudo-spin conservation in scattering within a smooth disorder potential.2,3 Topological lattice defects break the sublattice symmetry, allowing insight into the fundamental quantum properties of graphene. -
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. -
Ceramics Overview: Classification by Microstructure and Processing Methods
Clinical Ceramics overview: classification by microstructure and processing methods Edward A. McLaren 1 and Russell Giordano 2 Abstract The plethora of ceramic systems available today for all types of indirect restorations can be confusing and overwhelming for the clinician. Having a better understanding of them is important. In this article, the authors use classification systems based on microstructural components of ceramics and the processing techniques to help illustrate the various properties. Introduction component atoms, and may exhibit ionic or covalent Many different types of ceramic systems have been bonding. Although ceramics can be very strong, they are also introduced in recent years for all types of indirect extremely brittle and will catastrophically fail after minor restorations, from very conservative nonpreparation veneers, flexure. Thus, these materials are strong in compression but to multi-unit posterior fixed partial dentures and everything weak in tension. in between. Understanding all the different nuances of Contrast that with metals: metals are non-brittle (display materials and material processing systems is overwhelming elastic behaviour) and ductile (display plastic behaviour). This and can be confusing. This article will cover what types of is because of the nature of the interatomic bonding, which is ceramics are available based on a classification of the called metallic bonds; a cloud of shared electrons that can microstructural components of the ceramic. A second, easily move when energy is applied defines these bonds. This simpler classification system based on how the ceramics are is what makes most metals excellent conductors. Ceramics can processed will give the main guidelines for their use. be very translucent to very opaque. -
Texture and Microstructure
Texture and Microstructure • Microstructure contains far more than qualitative descriptions (images) of cross-sections of materials. • Most properties are anisotropic •it is important to quantitatively characterize the microstructure including orientation information (texture). In latin, textor means weaver In materials science, texture way in which a material is woven. Polycrystalline material is constituted from a large number of small crystallites (limited volume of material in which periodicity of crystal lattice is present). Each of these crystallites has a specific orientation of the crystal lattice. A randomly texture sheet A strongly textured sheet The cube texture (001) ND (Sheet Normal Direction) [100] RD (Sheet Rolling Direction) Crystallographic texture is the orientation distribution of crystallites in a polycrystalline material Texture :Metallurgists and Materials Scientists Fabric :Geologists and Mineralogists Preferred Orientation :Everybody Why textures? Texture influences the following properties: •Elastic modulus •Yield strength •Tensile ductility and strength •Formability •Fatigue strength •Fracture toughness •Stress corrosion cracking •Electrical and Magnetic properties Major fields of application A. Conventional • Aluminium industry • Steel industry • LC steels • Electrical steels • Titanium alloys • Zirconium base nuclear grade alloys B. Modern • High Tc superconductors • Thin films for semiconducting and magnetic devices • Bulk magnetic materials • Structural Ceramics • Polymers Beverage Cans Aluminium beverage -
Effects of Sio2/Al2o3 Ratios on Sintering Characteristics of Synthetic Coal Ash
Article Effects of SiO2/Al2O3 Ratios on Sintering Characteristics of Synthetic Coal Ash Hongwei Hu 1, Kun Zhou 1, Kesheng Meng 1,2, Lanbo Song 1 and Qizhao Lin 1,* 1 Department of Thermal Science and Energy Engineering, University of Science and Technology of China, Hefei 230027, China; [email protected] (H.H.); [email protected] (K.Z.); [email protected] (K.M.); [email protected] (L.S.) 2 Anhui Civil Aviation Airport Group, Hefei 230086, China * Correspondence: [email protected]; Tel.: +86-551-6360-0430; Fax: +86-551-6360-3487 Academic Editor: Mehrdad Massoudi Received: 01 December 2016; Accepted: 14 February 2017; Published: 16 February 2017 Abstract: This article explores the effects of SiO2/Al2O3 ratios (S/A) on sintering characteristics and provides guidance for alleviating ash depositions in a large-scale circulation fluidized bed. Five synthetic coal ash (SCA) samples with different S/As were treated in a muffle furnace for 12 h at different temperatures (from 773 K to 1373 K, in 100 K intervals). The morphological and chemical results of the volume shrinkage ratio (VSR), thermal deformation analysis by dilatometer (DIL), scanning electron microscope (SEM), X-ray photoelectron spectrometer (XPS), and X-ray diffraction (XRD) were combined to describe the sintering characteristics of different samples. The results showed that the sintering procedure mainly occurred in the third sintering stage when the temperature was over 1273 K, accompanied with significant decreases in the VSR curve. Excess SiO2 (S/A = 4.5) resulted in a porous structure while excess Al2O3 (S/A = 0.5) brought out large aggregations. -
Phase Field Modelling of Abnormal Grain Growth
materials Article Phase Field Modelling of Abnormal Grain Growth Ying Liu 1, Matthias Militzer 1,* and Michel Perez 2 1 The Centre for Metallurgical Process Engineering, The University of British Columbia, Vancouver, BC V6T1Z4, Canada; [email protected] 2 MATEIS, UMR CNRS 5510, INSA Lyon, Univ. Lyon, F69621 Villeurbanne, France; [email protected] * Correspondence: [email protected]; Tel.: +1-604-822-3676 Received: 20 October 2019; Accepted: 27 November 2019; Published: 5 December 2019 Abstract: Heterogeneous grain structures may develop due to abnormal grain growth during processing of polycrystalline materials ranging from metals and alloys to ceramics. The phenomenon must be controlled in practical applications where typically homogeneous grain structures are desired. Recent advances in experimental and computational techniques have, thus, stimulated the need to revisit the underlying growth mechanisms. Here, phase field modelling is used to systematically evaluate conditions for initiation of abnormal grain growth. Grain boundaries are classified into two classes, i.e., high- and low-mobility boundaries. Three different approaches are considered for having high- and low-mobility boundaries: (i) critical threshold angle of grain boundary disorientation above which boundaries are highly mobile, (ii) two grain types A and B with the A–B boundaries being highly mobile, and (iii) three grain types, A, B and C with the A–B boundaries being fast. For these different scenarios, 2D simulations have been performed to quantify the effect of variations in the mobility ratio, threshold angle and fractions of grain types, respectively, on the potential onset of abnormal grain growth and the degree of heterogeneity in the resulting grain structures. -
Nanoparticle Sintering
Application Note Nanoparticle Sintering Introduction the catalyst to be studied, and (iii) is observed (Fig. 2a). Analysis of Δλ preventing the catalyst from directly during the course of the experiment, Catalyst sintering is a major cause of interacting with the Au nanodisks by shows that the LSPR shifts fast in catalyst deactivation, which yearly e.g. alloy formation. the beginning and then more slowly causes billions of dollars of extra cost The Pt model catalyst is formed onto towards the end of the experiment associated with catalyst regeneration the sensor chip by evaporating a 0.5 (Fig. 2b, black curve). In contrast, and renewal. nm thick (nominal thickness) granu- when the same experiment is per- In order to develop more sintering- lar film. This results in individual Pt formed in pure Ar (or in 4% O2 on resistant catalysts, a detailed under- nanoparticles with an average diam- a “blank” sensor without Pt) no standing of the sintering kinetics and eter of <D> = 3.3 nm (+/- 1.1 nm), significant shift during the entire ex- mechanisms is required. It is therefore which mimics the size range of real periment is observed (Fig. 2b, blue of great importance to investigate sin- supported catalysts. curve). These results indicate that tering in situ, in real time and under The change of the localized surface INPS can be used to monitor the realistic catalyst operation conditions plasmon resonance (LSPR) centroid sintering of nanoparticle catalysts (i.e. at high temperatures and pres- wavelength, Δλ, is monitored during (since O2 is a known sintering pro- sures in reactive gas atmospheres). -
High Density Sintering of Ikon-Carbon Alloys Via
TWO-WEEK lOAN COPY This a Ubrar~ Circulating Cop~ which rna~ be borrowed for two weeks. For a personal retention cop~, call Tech. Info. Dioision, Ext. 6782 LBL tf8001 HIGH DENSITY SINTERING OF IRON-CARBON ALLOYS VIA TRANSIENT LIQUID PHASE Tin Tseuk Lam Materials and Molecular Research Division Lawrence Berkeley Laboratory and Department of Mechanical Engineering University of California Berkeley, California 94720 June 1978 HIGH DENSITY SINTERING OF IRON-CARBON ALLOYS VIA TRANSIENT LIQUID PHASE Abstract • , . v I. Introduction 1 II. Experimental Procedure 4 III. Experimental Results and Discussion . ' 8 IV. Conclusions 11 Acknowledgement , 12 References 13 Figure Captions 14 Figures 17 HIGH DENSITY SINTERING OF IRON~CARBON ALLOYS VIA TRANSIENT LIQUID PHASE Tin Tseuk Lam Materials and Molecular Research Division Lawrence Berkeley Laboratory and Department of Mechanical Engineering Uni vers1ty of California Berkeley, California 94720 ABSTRACT Because of the transient presence of a liquid phase during sintering of graphite coated iron powder, a high percentage (95% ~ 99.4%) of theoretical density can be achieved in a short time ( -10 min.) and at a moderate temperature (1175°C). As a result, the mechanical properties of the graphite coated sintered steel are close to those of commercial plain carbon steels and much better than those of commercial powder metallurgy sintered steels. In addition, the physical and mechanical properties of Fe 2%C 20%W were studied in the as~sintered condition. I Introduction The primary objective of this research project was to develop iron base materials with useful mechanical properties via a practical powder metallurgical process. Steels are very useful engineering materials. -
Development of the Microstructure of the Silicon Nitride Based Ceramics
Materials Research, Vol. 2, No. 3, 165-172, 1999. © 1999 Development of the Microstructure of the Silicon Nitride Based Ceramics J.C. Bressiani, V. Izhevskyi*, Ana H. A. Bressiani Instituto de Pesquisas Energéticas e Nucleares, IPEN, C.P. 11049 Pinheiros 05422-970 São Paulo - SP, Brazil Received: August 15, 1998; Revised: March 30, 1999 Basic regularities of silicon nitride based materials microstructure formation and development in interrelation with processing conditions, type of sintering additives, and starting powders properties are discussed. Models of abnormal or exaggerated grain growth are critically reassessed. Results of several model experiments conducted in order to determine the most important factors directing the microstructure formation processes in RE-fluxed Si3N4 ceramics are reviewed. Existing data on the mechanisms governing the microstructure development of Si3N4-based ceramics are analyzed and several principles of microstructure tailoring are formulated. Keywords: silicon nitride, microstructure, phase transformation, liquid phase sintering 1. Introduction the Weibull modulus of the fracture strength of silicon nitride. A small transverse grain size was shown to give Mechanical properties of the Si3N4-based ceramics higher Weibull modulus than the coarse microstructures. such as strength and fracture toughness as well as Weibull The observed increase in fracture resistance was mainly modulus are strongly dependent on the microstructure. attributed to crack deflection, and crack bridging mecha- Formation of the resulting microstructure is dictated by the nism3-6. In some cases crack branching was also observed. densification mechanism, i.e., reactive liquid phase sinter- An important role in fracture resistance improvement is ing. The α-Si3N4 in the starting powder compact is trans- played also by the secondary phase. -
Introduction to Material Science and Engineering Presentation.(Pdf)
Introduction to Material Science and Engineering Introduction What is material science? Definition 1: A branch of science that focuses on materials; interdisciplinary field composed of physics and chemistry. Definition 2: Relationship of material properties to its composition and structure. What is a material scientist? A person who uses his/her combined knowledge of physics, chemistry and metallurgy to exploit property-structure combinations for practical use. What are materials? What do we mean when we say “materials”? 1. Metals 2. Ceramics 3. Polymers 4. Composites - aluminum - clay - polyvinyl chloride (PVC) - wood - copper - silica glass - Teflon - carbon fiber resins - steel (iron alloy) - alumina - various plastics - concrete - nickel - quartz - glue (adhesives) - titanium - Kevlar semiconductors (computer chips, etc.) = ceramics, composites nanomaterials = ceramics, metals, polymers, composites Length Scales of Material Science • Atomic – < 10-10 m • Nano – 10-9 m • Micro – 10-6 m • Macro – > 10-3 m Atomic Structure – 10-10 m • Pertains to atom electron structure and atomic arrangement • Atom length scale – Includes electron structure – atomic bonding • ionic • covalent • metallic • London dispersion forces (Van der Waals) – Atomic ordering – long range (metals), short range (glass) • 7 lattices – cubic, hexagonal among most prevalent for engineering metals and ceramics • Different packed structures include: Gives total of 14 different crystalline arrangements (Bravais Lattices). – Primitive, body-centered, face-centered Nano Structure – 10-9 m • Length scale that pertains to clusters of atoms that make up small particles or material features • Show interesting properties because increase surface area to volume ratio – More atoms on surface compared to bulk atoms – Optical, magnetic, mechanical and electrical properties change Microstructure – 10-6 • Larger features composed of either nanostructured materials or periodic arrangements of atoms known as crystals • Features are visible with high magnification in light microscope.