Advanced Measurements of Silicon Carbide Ceramic Matrix Composites
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2.1.5 Stress-Strain Relation for Anisotropic Materials
,/... + -:\ 2.1.5Stress-strain Relation for AnisotropicMaterials The generalizedHook's law relatingthe stressesto strainscan be writtenin the form U2, 13,30-32]: o,=C,,€, (i,i =1,2,.........,6) Where: o, - Stress('ompttnents C,, - Elasticity matrix e,-Straincomponents The material properties (elasticity matrix, Cr) has thirty-six constants,stress-strain relations in the materialcoordinates are: [30] O1 LI CT6 a, l O2 03_ a, -t ....(2-6) T23 1/ )1 T32 1/1l 'Vt) Tt2 C16 c66 I The relations in equation (3-6) are referred to as characterizing anisotropicmaterials since there are no planes of symmetry for the materialproperties. An alternativename for suchanisotropic material is a triclinic material. If there is one plane of material property symmetry,the stress- strainrelations reduce to: -'+1-/ ) o1 c| ct2 ct3 0 0 crc €l o2 c12 c22 c23 0 0 c26 a: ct3 C23 ci3 0 0 c36 o-\ o3 ....(2-7) 723 000cqqc450 y)1 T3l 000c4sc5s0 Y3l T1a ct6 c26 c36 0 0 c66 1/t) Where the plane of symmetryis z:0. Such a material is termed monoclinicwhich containstfirfen independentelastic constants. If there are two brthogonalplanes of material property symmetry for a material,symmetry will existrelative to a third mutuallyorthogonal plane. The stress-strainrelations in coordinatesaligned with principal material directionswhich are parallel to the intersectionsof the three orthogonalplanes of materialsymmetry, are'. Ol ctl ct2ctl000 tl O2 Ct2 c22c23000 a./ o3 ct3 c23c33000 * o-\ ....(2-8) T23 0 00c4400 y)1 yll 731 0 000css0 712 0 0000cr'e 1/1) 'lt"' -' , :t i' ,/ Suchmaterial is calledorthotropic material.,There is no interaction betweennormal StreSSeS ot r 02, 03) andanisotropic materials. -
Ceramic Matrix Composites Taking Flight at GE Aviation Featuring
AMERICAN CERAMIC SOCIETY bullemerginge ceramicstin & glass technology APRIL 2019 Ceramic matrix composites taking flight at GE Aviation Featuring: April 30 – May 1, 2019 Ceramic science in the skies: Electrification, EBCs, and PDCs | New Ohio partnership for technician training FIRING YOUR IMAGINATION FOR 100 YEARS Ads from the 1940’s and 1950’s www.harropusa.com ACerS Anniversary Ad 2.indd 1 2/13/19 3:44 PM contents April 2019 • Vol. 98 No.3 feature articles Ceramic matrix composites taking flight at 30 GE aviation The holy grail for jet engines is efficiency, and the improved high-temperature capability of CMC systems is giving General Electric a great advantage. department News & Trends . 4 by Jim Steibel Spotlight . 10 Ceramics in Energy . 19 cover story Research Briefs . 21 Nonoxide polymer-derived CMCs for 34 “super” turbines The melting point of single-crystal blades limits further columns advancement in operating temperature of gas turbines with metallic materials. Ceramics, which have much higher melt- All about aircraft . 29 ing points, hold the promise for future “super” turbines. Infographic by Lisa McDonald by Zhongkan Ren and Gurpreet Singh Deciphering the Discipline . 64 Ultra-high temperature oxidation of high entropy UHTCs Taking off: Advanced materials contribute by Lavina Backman 40 to the evolution of electrified aircraft Commercial electrified aircraft are expected to take off within the next decade—and advanced materials are play- ing an increasingly critical role in solving key technical challenges that will push the boundaries even higher. meetings 25th International Congress on by Ajay Misra Glass (ICG 2019) . 56 GFMAT-2/Bio-4 . -
Nanomaterials How to Analyze Nanomaterials Using Powder Diffraction and the Powder Diffraction File™
Nanomaterials How to analyze nanomaterials using powder diffraction and the Powder Diffraction File™ Cerium Oxide CeO2 PDF 00-064-0737 7,000 6,000 5,000 4,000 Intensity 3,000 2,000 1,000 20 30 40 50 60 70 80 90 100 110 120 Nanomaterials Table of Contents Materials with new and incredible properties are being produced around the world by controlled design at the atomic and molecular level. These nanomaterials are typically About the Powder Diffraction File ......... 1 produced in the 1-100 nm size scale, and with this small size they have tremendous About Powder Diffraction ...................... 1 surface area and corresponding relative percent levels of surface atoms. Both the size and available (reactive) surface area can contribute to unique physical properties, Analysis Tools for Nanomaterials .......... 1 such as optical transparency, high dissolution rate, and enormous strength. Crystallite Size and Particle Size ������������ 2 In this Technical Bulletin, we are primarily focused on the use of structural simulations XRPD Pattern for NaCI – An Example .... 2 in order to examine the approximate crystallite size and molecular orientation in nanomaterials. The emphasis will be on X-ray analysis of nanomaterials. However, Total Pattern Analysis and the �������������� 3 Powder Diffraction File electrons and neutrons can have similar wavelengths as X-rays, and all of the X-ray methods described have analogs with neutron and electron diffraction. The use of Pair Distribution Function Analysis ........ 3 simulations allows one to study any nanomaterials that have a known atomic and Amorphous Materials ............................ 4 molecular structure or one can use a characteristic and reproducible experimental diffraction pattern. -
Particle Size and Structural Effects in Platinum Electrocatalysis
JOURNAL OF APPLIED ELECTROCHEMISTRY 20 (1990) 537-548 REVIEWS OF APPLIED ELECTROCHEMISTRY 23 Particle size and structural effects in platinum electrocatalysis S. MUKERJEE Tata Energy Research Institute, 7 Jor Bagh, New Delhi-llO 003, India Received 4 January 1989; revised 18 October 1989 Of the several factors which influence electrocatalytic activity, particle size and structural effects are of crucial importance, but their effects and mechanism of interaction, vis-a-vis overall performance, have been, at best, vaguely understood. The situation is further aggravated by the use of a wide range of experimental conditions resulting in non-comparable data. This paper attempts systematically to present the developments to date in the understanding of these structural interactions and to point out areas for future investigation. The entire content of this review has been examined from the context of the highly dispersed Pt electrocatalyst, primarily because it has been examined in the greatest detail. In the first two sections a general idea on the correlations between surface microstructure and geometric model is presented. Subsequently, indicators of a direct correlation between particle size and catalyst support synergism are considered. The structural and particle size effect on electro- catalysis is examined from the point of view of anodic hydrogen oxidation and cathodic oxygen reduction reactions. The hydrogen and oxygen chemisorption effects, presented with the discussion on the anodic and cathodic electrocatalytic reactions, provide important clues toward resolving some of the controversial findings, especially on the dependence of particle size on the anodic hydrogen oxidation reaction. Finally, the effect of alloy formation on the cathodic oxygen reduction reaction is discussed, providing insights into the structural aspect. -
Preparation of a Ceramic Matrix Composite Made of Hydroxyapatite Nanoparticles and Polylactic Acid by Consolidation of Composite Granules
nanomaterials Article Preparation of a Ceramic Matrix Composite Made of Hydroxyapatite Nanoparticles and Polylactic Acid by Consolidation of Composite Granules Elzbieta Pietrzykowska 1,2,*, Barbara Romelczyk-Baishya 2 , Jacek Wojnarowicz 1 , Marina Sokolova 3, Karol Szlazak 2, Wojciech Swieszkowski 2, Janis Locs 3 and Witold Lojkowski 1 1 Institute of High Pressure Physics, Polish Academy of Science, Sokolowska 29/37, 01-142 Warsaw, Poland; [email protected] (J.W.); [email protected] (W.L.) 2 Faculty of Materials Science and Engineering, Warsaw University of Technology, Woloska 141, 02-507 Warsaw, Poland; [email protected] (B.R.-B.); [email protected] (K.S.); [email protected] (W.S.) 3 Rudolfs Cimdins Riga Biomaterials Innovations and Development Centre of RTU, Institute of General Chemical Engineering, Faculty of Materials Science and Applied Chemistry, Riga Technical University, Pulka Street 3, LV-1007 Riga, Latvia; [email protected] (M.S.); [email protected] (J.L.) * Correspondence: [email protected]; Tel.: +48-228-760-429 Received: 31 March 2020; Accepted: 15 May 2020; Published: 30 May 2020 Abstract: Composites made of a biodegradable polymer, e.g., polylactic acid (PLA) and hydroxyapatite nanoparticles (HAP NPs) are promising orthopedic materials. There is a particular need for biodegradable hybrid nanocomposites with strong mechanical properties. However, obtaining such composites is challenging, since nanoparticles tend to agglomerate, and it is difficult to achieve good bonding between the hydrophilic ceramic and the hydrophobic polymer. This paper describes a two-step technology for obtaining a ceramic matrix composite. The first step is the preparation of composite granules. -
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. -
The Proposed Crystallization Behavior of the Teo2-Nb2o5-Bi2o3-Er2o3
The Proposed Crystallization Behavior of the TeO2-Nb2O5-Bi2O3-Er2O3 Glass Ceramic System By Cooper Howard An Honors Thesis Submitted In Partial Fulfillment of the Requirements For the Alfred University Honors Program Under the Supervision of: Chair: Dr. Yiquan Wu Committee Members: Dr. Holly Shulman, Dr. William LaCourse Alfred, NY May 2020 The road to completing this thesis began quite a long time ago, though its actual inception was fairly recent. When I began my time at Alfred University I was entered as a mechanical engineer, I went through all of the first year courses, and then got to our explorations in the second semester. I took the one on mechanical engineering first, I found myself becoming increasingly disinterested as the class went on, disillusioned with mechanical engineering. Then, I took the ceramics exploration, and it clicked. At the beginning of the next semester after the summer, I signed the paperwork and changed my major, and found my home in the world of materials science. Ceramic engineering immediately became something I was deeply interested in, I approached all the relevant coursework with gusto and a desire to learn. My excitement grew more and more as I realized how much of an active field the discipline is, the opportunities for research and discovery at every turn. This was the first key moment in how I came to my thesis. While my love for ceramic engineering grew, I also continued to cultivate my long held interest in physics, taking a physics course in every semester up until my senior year, where my workload finally caught up with me. -
Lecture II Polarization Anisotropy Spectrum
Lecture II Polarization Anisotropy Spectrum Wayne Hu Crete, July 2008 Damping Tail Dissipation / Diffusion Damping • Imperfections in the coupled fluid → mean free path λC in the baryons • Random walk over diffusion scale: geometric mean of mfp & horizon λD ~ λC√N ~ √λCη >> λC • Overtake wavelength: λD ~ λ ; second order in λC/λ • Viscous damping for R<1; heat conduction damping for R>1 1.0 N=η / λC Power λD ~ λC√N 0.1 perfect fluid instant decoupling λ 500 1000 1500 Silk (1968); Hu & Sugiyama (1995); Hu & White (1996) l Dissipation / Diffusion Damping • Rapid increase at recombination as mfp ↑ • Independent of (robust to changes in) perturbation spectrum • Robust physical scale for angular diameter distance test (ΩK, ΩΛ) Recombination 1.0 Power 0.1 perfect fluid instant decoupling recombination 500 1000 1500 Silk (1968); Hu & Sugiyama (1995); Hu & White (1996) l Damping • Tight coupling equations assume a perfect fluid: no viscosity, no heat conduction • Fluid imperfections are related to the mean free path of the photons in the baryons −1 λC = τ_ where τ_ = neσT a is the conformal opacity to Thomson scattering • Dissipation is related to the diffusion length: random walk approximation p p p λD = NλC = η=λC λC = ηλC the geometric mean between the horizon and mean free path • λD/η∗ ∼ few %, so expect the peaks :> 3 to be affected by dissipation Equations of Motion • Continuity k Θ_ = − v − Φ_ ; δ_ = −kv − 3Φ_ 3 γ b b where the photon equation remains unchanged and the baryons follow number conservation with ρb = mbnb • Euler k v_ = k(Θ + Ψ) − π − τ_(v − v ) γ 6 γ γ b a_ v_ = − v + kΨ +τ _(v − v )=R b a b γ b where the photons gain an anisotropic stress term πγ from radiation viscosity and a momentum exchange term with the baryons and are compensated by the opposite term in the baryon Euler equation Viscosity • Viscosity is generated from radiation streaming from hot to cold regions • Expect k π ∼ v γ γ τ_ generated by streaming, suppressed by scattering in a wavelength of the fluctuation. -
Effect of Heat Treatment on the Activity and Stability of Carbon Supported Ptmo Alloy Electrocatalysts for Hydrogen Oxidation in Proton Exchange Membrane Fuel Cells
Journal of Power Sources 247 (2014) 712e720 Contents lists available at ScienceDirect Journal of Power Sources journal homepage: www.elsevier.com/locate/jpowsour Effect of heat treatment on the activity and stability of carbon supported PtMo alloy electrocatalysts for hydrogen oxidation in proton exchange membrane fuel cells Ayaz Hassan a, Alejo Carreras b, Jorge Trincavelli b, Edson Antonio Ticianelli a, * a Instituto de Quimica de São Carlos, Universidade de São Paulo, Caixa Postal 7 80, São Carlos, SP CEP 13560-970, Brazil b Instituto de Física Enrique Gaviola (IFEG)-CONICET, Facultad de Matemática, Astronomía y Física, Universidad Nacional de Córdoba, Medina Allende s/n, 5016 Córdoba, Argentina highlights The CO tolerance and stability of heat-treated carbon supported PtMo (60:40 at.%) catalysts are investigated. The PtMo/C catalyst treated at 600 C shows higher CO tolerance compared to that of the untreated material. PtMo/C electrocatalysts suffer a partial dissolution of Mo during a 5000 times cycling aging. The stability of the PtMo/C electrocatalyst is improved after the 600 C heating treatment. article info abstract Article history: The effect of heat treatment on the activity, stability and CO tolerance of PtMo/C catalysts was studied, Received 20 July 2013 due to their applicability in the anode of proton exchange membrane fuel cells (PEMFCs). To this purpose, Received in revised form a carbon supported PtMo (60:40) alloy electrocatalyst was synthesized by the formic acid reduction 29 August 2013 method, and samples of this catalyst were heat-treated at various temperatures ranging between 400 Accepted 31 August 2013 and 700 C. -
Cosmic Microwave Background
1 29. Cosmic Microwave Background 29. Cosmic Microwave Background Revised August 2019 by D. Scott (U. of British Columbia) and G.F. Smoot (HKUST; Paris U.; UC Berkeley; LBNL). 29.1 Introduction The energy content in electromagnetic radiation from beyond our Galaxy is dominated by the cosmic microwave background (CMB), discovered in 1965 [1]. The spectrum of the CMB is well described by a blackbody function with T = 2.7255 K. This spectral form is a main supporting pillar of the hot Big Bang model for the Universe. The lack of any observed deviations from a 7 blackbody spectrum constrains physical processes over cosmic history at redshifts z ∼< 10 (see earlier versions of this review). Currently the key CMB observable is the angular variation in temperature (or intensity) corre- lations, and to a growing extent polarization [2–4]. Since the first detection of these anisotropies by the Cosmic Background Explorer (COBE) satellite [5], there has been intense activity to map the sky at increasing levels of sensitivity and angular resolution by ground-based and balloon-borne measurements. These were joined in 2003 by the first results from NASA’s Wilkinson Microwave Anisotropy Probe (WMAP)[6], which were improved upon by analyses of data added every 2 years, culminating in the 9-year results [7]. In 2013 we had the first results [8] from the third generation CMB satellite, ESA’s Planck mission [9,10], which were enhanced by results from the 2015 Planck data release [11, 12], and then the final 2018 Planck data release [13, 14]. Additionally, CMB an- isotropies have been extended to smaller angular scales by ground-based experiments, particularly the Atacama Cosmology Telescope (ACT) [15] and the South Pole Telescope (SPT) [16]. -
Use of High Energy Ball Milling on the Sintering Optimization of Alumina Ceramics
Seventh International Latin American Conference on Powder Technology, November 08-10, Atibaia, SP, Brazil Use of high energy ball milling on the sintering optimization of alumina ceramics Helio R. Simoni1,a, Eduardo Saito1,b, Claudinei dos Santos1,2,c, Felipe Antunes Santos1,d, Alfeu Saraiva Ramos3,e, Olivério Moreira M.Silva4,f 1 USP-EEL - Universidade de São Paulo, Escola de Engenharia de Lorena, Polo Urbo Industrial, Gleba AI6, s/n, Mondesir, Lorena-SP, Brazil, CEP12600-000 2UNIFOA - Centro Universitário de Volta Redonda, Av. Paulo Erlei Alves Abrantes, 1325, Volta Redonda-RJ, Brazil, CEP 27240-560 3 UNESP-FEG - Unersidade Estadual Paulista, Faculdade de Engenharia de Guaratinguetá, Av. Dr. Ariberto Pereirada Cunha, 333, Guaratinguetá-SP, Brazil, CEP 12516-410 4 CTA-IAE/AMR - Centro Técnico Aeroespacial, Praça Marechal do Ar Eduardo Gomes, 50, S.J. Campos-SP, Brazil, CEP 12228-904 [email protected], [email protected], [email protected], [email protected], [email protected] Keywords: Al2O3, Al2O3-Y2O3, high-energy ball milling, sintering, characterization Abstract: In this work, the effect of the milling time on the densification of the alumina ceramics with or without 5wt.%Y2O3, is evaluated, using high-energy ball milling. The milling was performed with different times of 0, 2, 5 or 10 hours. All powders, milled at different times, were characterized by X-Ray Diffraction presenting a reduction of the crystalline degree and crystallite size as function of the milling time increasing. The powders were compacted by cold uniaxial pressing and sintered at 1550°C-60min. Green density of the compacts presented an increasing as function of the milling time and sintered samples presented evolution on the densification as function of the reduction of the crystallite size of the milled powders. -
Development of New Matrix and Interfacial Materials for Ceramic Matrix Composites Gavin C
University of Connecticut OpenCommons@UConn Doctoral Dissertations University of Connecticut Graduate School 8-26-2014 Development of New Matrix and Interfacial Materials for Ceramic Matrix Composites Gavin C. Richards University of Connecticut - Storrs, [email protected] Follow this and additional works at: https://opencommons.uconn.edu/dissertations Recommended Citation Richards, Gavin C., "Development of New Matrix and Interfacial Materials for Ceramic Matrix Composites" (2014). Doctoral Dissertations. 522. https://opencommons.uconn.edu/dissertations/522 Development of New Matrix and Interfacial Materials for Ceramic Matrix Composites Gavin C. Richards, PhD University of Connecticut, 2014 Pre-ceramic polymers are attractive, low cost materials for the manufacture of ceramic fibers and matrix materials in Ceramic Matrix Composites (CMCs). A new pre-ceramic polymer, an ethanol-modified polyvinylsilazane (PVSZ), was synthesized and characterized. The PVSZ polymer has been previously shown to be a viable precursor for silicon nitride and silicon carbide based ceramics, but lacked stability when exposed to air. The PVSZ polymer was synthesized via the ammonolysis of trichlorovinylsilazane in tetrahydrofuran (THF), and then reacted with ethanol to form the ethanol-modified PVSZ. The PVSZ polymer and ethanol- modified PVSZ resin were each characterized with Attenuated Total Reflectance spectroscopy (ATR), 1H Nuclear Magnetic Resonance ( 1H-NMR), and Gel Permeation Chromatography (GPC), Thermogravimetric Analysis (TGA), Residual Gas Analysis (RGA), and X-Ray Powder Diffraction (XRD) of the ceramic char after pyrolysis in various atmospheres. A second new modified PVSZ was also synthesized. Rather than use ethanol, a second silane monomer was added during synthesis, with the intent of stabilizing the polymer without incorporating oxygen. The new end cap modified PVSZ (EC-PVSZ) was characterized using the same methods outlined for the ethanol-modified PVSZ.