Exploring the Surface Properties of the Liquid Metals
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Low-Temperature Specific Heat in Caesium Borate Glasses Cristina Crupi, Giovanna D’Angelo, Gaspare Tripodo, Giuseppe Carini, A
Low-temperature specific heat in caesium borate glasses Cristina Crupi, Giovanna d’Angelo, Gaspare Tripodo, Giuseppe Carini, A. Bartolotta To cite this version: Cristina Crupi, Giovanna d’Angelo, Gaspare Tripodo, Giuseppe Carini, A. Bartolotta. Low- temperature specific heat in caesium borate glasses. Philosophical Magazine, Taylor & Francis, 2007, 87 (3-5), pp.741-747. 10.1080/14786430600910764. hal-00513746 HAL Id: hal-00513746 https://hal.archives-ouvertes.fr/hal-00513746 Submitted on 1 Sep 2010 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. Philosophical Magazine & Philosophical Magazine Letters For Peer Review Only Low-temperature specific heat in caesium borate glasses Journal: Philosophical Magazine & Philosophical Magazine Letters Manuscript ID: TPHM-06-May-0176.R1 Journal Selection: Philosophical Magazine Date Submitted by the 27-Jun-2006 Author: Complete List of Authors: Crupi, Cristina; Messina University, Physics D'Angelo, Giovanna; university of messina, physics Tripodo, Gaspare; Messina University, Physics carini, giuseppe; University of Messina, Dept of Physics Bartolotta, A.; Istituto per i Processi Chimico-Fisici, CNR amorphous solids, boson peak, calorimetry, disordered systems, Keywords: glass, specific heat, thermal properties Keywords (user supplied): http://mc.manuscriptcentral.com/pm-pml Page 1 of 13 Philosophical Magazine & Philosophical Magazine Letters 1 2 3 LOW TEMPERATURE SPECIFIC HEAT IN CAESIUM BORATE GLASSES 4 5 6 7 8 + 9 Cristina Crupi, Giovanna D’Angelo, Gaspare Tripodo, Giuseppe Carini and Antonio Bartolotta . -
(VI) and Chromium (V) Oxide Fluorides
Portland State University PDXScholar Dissertations and Theses Dissertations and Theses 1976 The chemistry of chromium (VI) and chromium (V) oxide fluorides Patrick Jay Green Portland State University Follow this and additional works at: https://pdxscholar.library.pdx.edu/open_access_etds Part of the Chemistry Commons Let us know how access to this document benefits ou.y Recommended Citation Green, Patrick Jay, "The chemistry of chromium (VI) and chromium (V) oxide fluorides" (1976). Dissertations and Theses. Paper 4039. https://doi.org/10.15760/etd.5923 This Thesis is brought to you for free and open access. It has been accepted for inclusion in Dissertations and Theses by an authorized administrator of PDXScholar. Please contact us if we can make this document more accessible: [email protected]. All ABSTRACT OF THE TllESIS OF Patrick Jay Green for the Master of Science in Chemistry presented April 16, 1976. Title: Chemistry of Chromium(VI) and Chromium(V) Oxide Fluorides. APPROVEO BY MEMBERS OF THE THESIS CO'"o\l TIEE: y . • Ii . ' I : • • • • • New preparative routes to chromyl fluoride were sought. It was found that chlorine ironofluoride reacts with chromium trioxide and chromyl chlo ride to produce chromyl fluoride. Attempts were ~ade to define a mechan ism for the reaction of ClF and Cr0 in light of by-products observed 3 and previous investigations. Carbonyl fluoride and chromium trioxide react to fom chro·yl fluoride and carbo:i dioxide. A mechanism was also proposed for this react10n. Chromium trioxide 11itl\ l~F6 or WF5 reacts to produce chromyl fluoride and the respective oxide tetrafluoride. 2 Sulfur hexafluoride did not react with Cr03. -
Influence of Composition on Structure and Caesium Volatilisation from Glasses for HLW Confinement
Influence of Composition on Structure and Caesium Volatilisation from Glasses for HLW Confinement Benjamin Graves Parkinson B.Sc. (Hons.), M.Sc. A thesis submitted to the University of Warwick in partial fulfilment of the requirement for the degree of Doctor of philosophy Department of Physics November 2007 Contents Contents (i) List of Figures (vi) List of Tables (xv) List of Abbreviations (xvii) Acknowledgements (xviii) Declaration (xix) Abstract (xx) Chapter 1...................................................................................................................1 1 Introduction....................................................................................................1 1.1 Overview................................................................................................1 1.2 Aim of the work .....................................................................................1 1.3 References..............................................................................................5 Chapter 2...................................................................................................................7 2 Immobilisation of High Level Nuclear Waste.................................................7 2.1 Introduction............................................................................................7 2.2 High-Level Nuclear Waste......................................................................7 2.3 HLW Immobilisation..............................................................................8 2.3.1 -
Effect of Gamma Radiation on Electrical and Optical Properties of (Teo2)0·9 (In2o3)0·1 Thin films
Bull. Mater. Sci., Vol. 34, No. 1, February 2011, pp. 61–69. c Indian Academy of Sciences. Effect of gamma radiation on electrical and optical properties of (TeO2)0·9 (In2O3)0·1 thin films S L SHARMA∗ and T K MAITY Department of Physics & Meteorology, Indian Institute of Technology, Kharagpur 721 302, India MS received 13 March 2010 Abstract. We have studied in detail the gamma radiation induced changes in the electrical properties of the (TeO2)0·9 (In2O3)0·1 thin films of different thicknesses, prepared by thermal evaporation in vacuum. The current– voltage characteristics for the as-deposited and exposed thin films were analysed to obtain current versus dose plots at different applied voltages. These plots clearly show that the current increases quite linearly with the radiation dose over a wide range and that the range of doses is higher for the thicker films. Beyond certain dose (a quantity dependent on the film thickness), however, the current has been observed to decrease. In order to understand the dose dependence of the current, we analysed the optical absorption spectra for the as-deposited and exposed thin films to obtain the dose dependences of the optical bandgap and energy width of band tails of the localized states. The increase of the current with the gamma radiation dose may be attributed partly to the healing effect and partly to the lowering of the optical bandgap. Attempts are on to understand the decrease in the current at higher doses. Employing dose dependence of the current, some real-time gamma radiation dosimeters have been prepared, which have been found to possess sensitivity in the range 5–55 μGy/μA/cm2. -
A Thesis for the Degree of Doctor of Philosophy The
A THESIS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY THE THERMAL DEGRADATION OF SOME POLYELECTROLYTES BY MUHAMMAD ZULFIQAR A SUPERVISOR: DR. I.C. McNEILL Chemistry Department, University of Glasgow. October, 1975. ProQuest Number: 13803963 All rights reserved INFORMATION TO ALL USERS The quality of this reproduction is dependent upon the quality of the copy submitted. In the unlikely event that the author did not send a complete manuscript and there are missing pages, these will be noted. Also, if material had to be removed, a note will indicate the deletion. uest ProQuest 13803963 Published by ProQuest LLC(2018). Copyright of the Dissertation is held by the Author. All rights reserved. This work is protected against unauthorized copying under Title 17, United States Code Microform Edition © ProQuest LLC. ProQuest LLC. 789 East Eisenhower Parkway P.O. Box 1346 Ann Arbor, Ml 4 8 1 0 6 - 1346 PREFACE The work described in this thesis was carried out during the period October 1971 to September 1974 at the University of Glasgow, in the Department of Physical Chemistry, which is under the supervision of Professor G.A. Sim. My thanks are due to my colleagues in the Macromolecular Chemistry group for invaluable assistance and discussion, and to various members of the technical staff of the Chemistry Department, in particular, Mr. J. Gorman and Mrs. F. Lawrie. Finally, I should like to thank my supervisor, Dr. I«C. McNeill, for suggesting the topic of this thesis, and for his advice and constant .encouragement throughout this work. SUMMARY All naturally occurring polyelectrolytes are found in an aqueous environment and this feature directed most of the chemical research in this field towards an understanding of polyelectrolyte behaviour in aqueous solution. -
A Study of Nickel Molybdenum Oxide Catalysts for The
A STUDY OF NICKEL MOLYBDENUM OXIDE CATALYSTS FOR THE OXIDATIVE DEHYDROGENATION OF n-HEXANE By Bavani Pillay Submitted in fulfilment of the academic requirements for the degree of Doctor of Philosophy in the School of Chemistry University of KwaZulu-Natal Durban, South Africa June 2009 As the candidate’s supervisor I have/have not approved this thesis/dissertation for submission. Signed: _____________ Name: _____________ Date: ______________ ii ABSTRACT Nickel molybdenum oxide catalysts with different chemical compositions have been synthesized and tested for the oxidative dehydrogenation of n-hexane. The co-precipitation method was used for the synthesis and several methods were used to characterize these catalysts. These include inductively-coupled plasma optical emission spectroscopy, Raman spectroscopy, infrared spectroscopy, energy dispersive X-ray spectroscopy, scanning electron microscopy, temperature programmed reduction, temperature programmed desorption, X-ray photo-electron spectroscopy and X-ray diffraction spectroscopy techniques as well as the Brauner-Emmet-Teller technique for surface area determination. The phase composition of the catalysts was largely dependent on the chemical composition. Catalyst testing on n-hexane feed was done with a fixed bed continuous flow reactor and experiments were performed with feed/air ratios above and below the flammability limit. Varied reaction conditions were used for the catalytic testing. Prior to the catalytic testing, blank experiments were performed. Analysis of the products were done both online and offline in conjunction with gas chromatography employing FID and TCD detectors. The influence of the catalyst on the conversion of n-hexane and selectivity to dehydrogenation products is reported. Products observed were the carbon oxides (CO and CO 2), isomers of hexene (1-hexene, 2-hexene and 3-hexene), cyclic C 6 products (cyclohexene and benzene), cracked products: alkanes/alkenes (propane/ene, butane/ene) and oxygenates (ethanal, acetic acid and propanoic acid). -
Luminescent Properties of Cdte Quantum Dots Synthesized Using 3-Mercaptopropionic Acid Reduction of Tellurium Dioxide Directly
Shen et al. Nanoscale Research Letters 2013, 8:253 http://www.nanoscalereslett.com/content/8/1/253 NANO EXPRESS Open Access Luminescent properties of CdTe quantum dots synthesized using 3-mercaptopropionic acid reduction of tellurium dioxide directly Mao Shen1*, Wenping Jia1, Yujing You1, Yan Hu2, Fang Li1,3, Shidong Tian3, Jian Li3, Yanxian Jin1 and Deman Han1 Abstract A facile one-step synthesis of CdTe quantum dots (QDs) in aqueous solution by atmospheric microwave reactor has been developed using 3-mercaptopropionic acid reduction of TeO2 directly. The obtained CdTe QDs were characterized by ultraviolet–visible spectroscopy, fluorescent spectroscopy, X-ray powder diffraction, multifunctional imaging electron spectrometer (XPS), and high-resolution transmission electron microscopy. Green- to red-emitting CdTe QDs with a maximum photoluminescence quantum yield of 56.68% were obtained. Keywords: CdTe quantum dots, 3-mercaptopropionic acid, TeO2, Microwave irradiation, Photoluminescence Background capping ligand for CdTe QDs. Such synthetic approach In recent years, water-soluble CdTe luminescent quantum eliminates the use of NaBH4 and allows facile one-pot dots (QDs) have been used in various medical and bio- synthesis of CdTe QDs. logical imaging applications because their optical proper- ties are considered to be superior to those of organic dyes [1-4]. Up to now, in most of the aqueous approaches, Te Methods Chemicals powder was used as the tellurium source and NaBH4 as the reductant, which needs a pretreatment to synthesize Tellurium dioxide (TeO2,99.99%),cadmiumchlor- the unstable tellurium precursor. The process of preparing ide hemi(pentahydrate) (CdCl2 ·2.5H2O, 99%), and 3-mercaptopropionic acid (MPA, 99%) were pur- CdTe QDs requires N2 as the protective gas at the initial chased from Aldrich Corporation (MO, USA). -
Chemical Formula of Binary Ionic Compounds – Sheet 1 the Combining Power Or Valency of Silver Is Always 1
Chemical Formula of Binary Ionic Compounds – Sheet 1 The combining power or valency of silver is always 1. All other transition metals are 2 unless otherwise indicated. No. Binary compound Formula No. Binary compound Formula 1 potassium fluoride 26 calcium sulfide 2 calcium chloride 27 lithium bromide 3 barium bromide 28 nickel sulfide 4 silver sulfide 29 zinc phosphide 5 aluminium iodide 30 barium iodide 6 potassium iodide 31 caesium chloride 7 lead(IV) oxide 32 copper bromide 8 zinc nitride 33 sodium nitride 9 silver iodide 34 silver chloride 10 barium fluoride 35 sodium hydride 11 lead(II) iodide 36 potassium nitride 12 silver fluoride 37 cobalt chloride 13 sodium sulfide 38 magnesium sulfide 14 sodium bromide 39 potassium chloride 15 calcium oxide 40 calcium bromide 16 zinc fluoride 41 iron(III) oxide 17 strontium phosphide 42 aluminium fluoride 18 barium sulfide 43 magnesium bromide 19 aluminium oxide 44 iron(III) chloride 20 aluminium chloride 45 barium nitride 21 aluminium sulfide 46 sodium fluoride 22 lead(II) oxide 47 lithium fluoride 23 barium chloride 48 lithium iodide 24 copper chloride 49 lithium hydride 25 barium phosphide 50 potassium oxide “Aluminum” and “cesium” are commonly used alternative spellings for "aluminium" and "caesium that are used in the US. May be freely copied for educational use. ©www.chemicalformula.org Chemical Formula of Binary Ionic Compounds – Sheet 2 The combining power or valency of silver is always 1. All other transition metals are 2 unless otherwise indicated. No. Binary compound Formula No. -
Normal Vibrations of Two Polymorphic Forms of Teo2 Crystals and Assignments of Raman Peaks of Pure Teo2 Glass
Nippon Seramikkusu Kyokai GakujutsuRonbunshi 97 [12] 1435-40 (1989) 1435 Normal Vibrations of Two Polymorphic forms of TeO2 Crystals and Assignments of Raman Peaks of Pure TeO2 Glass Takao SEKIYA, Norio MOCHIDA, Atsushi OHTSUKA and Mamoru TONOKAWA† ( Division of Materials Science and Chemical Engineering, Faculty of Engineering, Yokohama National University, 156, Tokiwadai, Hodogaya-ku, Yokohama-shi 240) TeO2結 晶 の 二 つ の 多 形 の 基 準 振 動 の 計 算 とTeO2ガ ラ ス の ラ マ ン ピ ー ク の 帰 属 関 谷 隆 夫 ・持 田 統 雄 ・大 塚 淳 ・殿 川 衛 † (横浜国立 大学工学部物質工学科, 240横 浜市保土 ケ谷区常盤台156) Raman spectra of paratellurite, tellurite and pure TeO2 glass were measured. The normal vibration of paratellurite and tellurite was analyzed. The spectrum of pure TeO2glass were deconvoluted into symmetric Gaussian functions. The normal vibrations of paratellurite are exactly described as combined representations of movement of oxygen atom in Te-eqOax-Te linkage and vibrations of TeO4 trigonal bipyramid (tbp). Compared the resolved Raman peaks of pure TeO2glass with nor mal vibration of paratellurite, all Raman peaks from 420 to 880 cm-1 are assigned to the vibrations of TeO4 tbp and Te-eqOax-Te linkage. The antisymmetric stretching vibrations of Te-qeOax-Te linkage have relatively large intensities to symmetric stretching vibrations of Te-eqOax-Te linkage. In pure TeO2 glass, TeO4 tops are formed by most of tellurium atoms and connected at vertices by the Te-eqOax-Te linkages. [ReceivedMay 18, 1989; AcceptedAugust 22, 1989] Key-words: Normal vibration, Raman spectrum, Paratellurite, Tellurite, Pure TeO2glass 1. -
Release of Fission Products During and After Oxidation of Trace-Irradiated Uranium Dioxide at 3Oo-9Oo°C
XA0056017 RELEASE OF FISSION PRODUCTS DURING AND AFTER OXIDATION OF TRACE-IRRADIATED URANIUM DIOXIDE AT 3OO-9OO°C P. Wood, G.H. Bannister Central Electricity Generating Board Berkeley Nuclear Laboratories UK Abstract Should defected U02 fuel pins come into contact with air then oxidation of the fuel may occur, the rate and consequences of which are dependent upon temperature and oxygen partial pressure. At CEGB-BNL an experimental programme is underway investigating the kinetics, and extent, of release of fission products during and after oxidation of trace-irradiated U02 to U3O3, and reduction of U3O3 to UO 2« This paper presents preliminary results and analysis of experiments performed at 300-900°C. Dense sintered U02 has been oxidised at 300-500°C using a thermobalance with simultaneous counting of released 85Kr. The kinetics of the 35Kr release are shown to correlate with the kinetics of oxidation, and the extent of release has been determined as 3-8% of that in the UO 2 converted to U3O3. The release of 106Ru and 137Cs during this oxidation has been estimated by Y~c°unting of the fuel sample, before and after oxidation, and of glassware in the vicinity of the sample. This indicates slight release of ruthenium and caesium. Greater fission product release is caused by oxidation at higher temperatures or by heating of the oxidation product. U 308 produced at 400°C has been heated at 800 and 900°C in air for 20 hours. This results in near total release of 85Kr and 106Ru, but still only slight release of 137Cs. -
Chemical Names and CAS Numbers Final
Chemical Abstract Chemical Formula Chemical Name Service (CAS) Number C3H8O 1‐propanol C4H7BrO2 2‐bromobutyric acid 80‐58‐0 GeH3COOH 2‐germaacetic acid C4H10 2‐methylpropane 75‐28‐5 C3H8O 2‐propanol 67‐63‐0 C6H10O3 4‐acetylbutyric acid 448671 C4H7BrO2 4‐bromobutyric acid 2623‐87‐2 CH3CHO acetaldehyde CH3CONH2 acetamide C8H9NO2 acetaminophen 103‐90‐2 − C2H3O2 acetate ion − CH3COO acetate ion C2H4O2 acetic acid 64‐19‐7 CH3COOH acetic acid (CH3)2CO acetone CH3COCl acetyl chloride C2H2 acetylene 74‐86‐2 HCCH acetylene C9H8O4 acetylsalicylic acid 50‐78‐2 H2C(CH)CN acrylonitrile C3H7NO2 Ala C3H7NO2 alanine 56‐41‐7 NaAlSi3O3 albite AlSb aluminium antimonide 25152‐52‐7 AlAs aluminium arsenide 22831‐42‐1 AlBO2 aluminium borate 61279‐70‐7 AlBO aluminium boron oxide 12041‐48‐4 AlBr3 aluminium bromide 7727‐15‐3 AlBr3•6H2O aluminium bromide hexahydrate 2149397 AlCl4Cs aluminium caesium tetrachloride 17992‐03‐9 AlCl3 aluminium chloride (anhydrous) 7446‐70‐0 AlCl3•6H2O aluminium chloride hexahydrate 7784‐13‐6 AlClO aluminium chloride oxide 13596‐11‐7 AlB2 aluminium diboride 12041‐50‐8 AlF2 aluminium difluoride 13569‐23‐8 AlF2O aluminium difluoride oxide 38344‐66‐0 AlB12 aluminium dodecaboride 12041‐54‐2 Al2F6 aluminium fluoride 17949‐86‐9 AlF3 aluminium fluoride 7784‐18‐1 Al(CHO2)3 aluminium formate 7360‐53‐4 1 of 75 Chemical Abstract Chemical Formula Chemical Name Service (CAS) Number Al(OH)3 aluminium hydroxide 21645‐51‐2 Al2I6 aluminium iodide 18898‐35‐6 AlI3 aluminium iodide 7784‐23‐8 AlBr aluminium monobromide 22359‐97‐3 AlCl aluminium monochloride -
Behaviour and Chemical State of Irradiated Ceramic Fuels
BEHAVIOUR AND CHEMICAL STATE OF IRRADIATED CERAMIC FUELS INTERNATIONAL ATOMIC ENERGY AGENCY, VIENNA, 1974 BEHAVIOUR AND CHEMICAL STATE OF IRRADIATED CERAMIC FUELS The following States are Members of the International Atomic Energy Agency: AFGHANISTAN HAITI PAKISTAN ALBANIA HOLY SEE PANAMA ALGERIA HUNGARY PARAGUAY ARGENTINA ICELAND PERU AUSTRALIA INDIA PHILIPPINES AUSTRIA INDONESIA POLAND BANGLADESH IRAN PORTUGAL -BELGIUM IRAQ ROMANIA BOLIVIA IRELAND SAUDI ARABIA BRAZIL ISRAEL SENEGAL BULGARIA ITALY SIERRA LEONE BURMA IVORY COAST SINGAPORE BYELORUSSIAN SOVIET JAMAICA SOUTH AFRICA SOCIALIST REPUBLIC JAPAN SPAIN CAMEROON JORDAN SRI LANKA CANADA KENYA SUDAN CHILE KHMER REPUBLIC . SWEDEN COLOMBIA KOREA, REPUBLIC OF SWITZERLAND COSTA RICA KUWAIT SYRIAN ARAB REPUBLIC CUBA LEBANON THAILAND CYPRUS LIBERIA TUNISIA CZECHOSLOVAK SOCIALIST LIBYAN ARAB REPUBLIC TURKEY REPUBLIC LIECHTENSTEIN UGANDA DENMARK LUXEMBOURG UKRAINIAN SOVIET SOCIALIST DOMINICAN REPUBLIC MADAGASCAR REPUBLIC ECUADOR MALAYSIA UNION OF SOVIET SOCIALIST EGYPT, ARAB REPUBLIC OF MALI REPUBLICS EL SALVADOR MEXICO UNITED KINGDOM OF GREAT ETHIOPIA MONACO BRITAIN AND NORTHERN FINLAND MONGOLIA IRELAND FRANCE MOROCCO UNITED STATES OF AMERICA GABON NETHERLANDS URUGUAY GERMAN DEMOCRATIC REPUBLIC NEW ZEALAND VENEZUELA GERMANY, FEDERAL REPUBLIC OF NIGER VIET-NAM GHANA NIGERIA YUGOSLAVIA GREECE NORWAY ZAIRE, REPUBLIC OF GUATEMALA ZAMBIA The Agency's Statute was approved on 23 October 1956 by the Conference on die Statute of the IAEA held at United Nations Headquarters, Mew York; it entered into force on 29 Iuly 1957, The Headquarters of the Agency are situated in Vienna. Its principal objective is "to accelerate and enlarge the contribution of atom ic energy to peace, health and prosperity throughout the world". © IAEA, 1974 Permission to reproduce or translate the information contained in this publication may be obtained by writing to the International Atomic Energy Agency, Kärntner Ring 11, P.O.