Nuclear and Space Radiation Effects on Materials
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The Radiation Challenge Module 2: Radiation Damage in Living Organisms Educator Guide
National Aeronautics and Space Administration Space Faring The Radiation Challenge An Interdisciplinary Guide on Radiation and Human Space Flight Module 2: Radiation Damage in Living Organisms Educational Product Educators Grades and Students 9 – 12 EP-2007-08-117-MSFC Radiation Educator Guide Module 2: Radiation Damage in Living Organisms Prepared by: Jon Rask, M.S., ARC Education Specialist Wenonah Vercoutere, Ph.D., NASA ARC Subject Matter Expert Al Krause, MSFC Education Specialist BJ Navarro, NASA ARC Project Manager Space Faring: The Radiation Challenge i Table of Contents Module 2: Module 2: Radiation Damage in Living Organisms .............................................................................1 Why is NASA Studying the Biological Effects of Radiation? .........................................................1 How Do Scientists Study Biological Change During Spaceflight? .................................................1 Using Non-Human Organisms to Understand Radiation Damage ................................................2 What are the Risks and Symptoms of Radiation Exposure for Humans? .......................................3 What is DNA? ..............................................................................................................................3 What is the Structure of DNA? .....................................................................................................3 What is DNA’s Role in Protein Production? ..................................................................................4 -
In0000721 Redistribution of Thermal X-Ray Radiation In
IN0000721 BARC/1999/E/043 CO > O CO to m o>»» REDISTRIBUTION OF THERMAL X-RAY RADIATION IN CAVITIES: VIEW-FACTOR METHOD AND COMPARISON WITH DSN CALCULATIONS by M.K. Srivastava Theoretical Physics Division and Vinod Kumar and S.V.G. Menon Solid State & Spectroscopy Group 31/30 1999 BARC/1999/E/043 GOVERNMENT OF INDIA ATOMIC ENERGY COMMISSION REDISTRIBUTION OF THERMAL X-RAY RADIATION IN CAVITIES: VIEW-FACTOR METHOD AND COMPARISON WITH DSN CALCULATIONS by M.K. Srivastava Theoretical Physics Division and Vinod Kumar and S.V.G. Menon Solid State & Spectroscopy Group BHABHA ATOMIC RESEARCH CENTRE MUMBAI, INDIA 1999 BARC/199S/E/043 BIBLIOGRAPHIC DESCRIPTION SHEET FOR TECHNICAL REPORT (as per IS : 9400 -1980) 01 Security classification: Unclassified 02 Distribution: External 03 Report status: New 04 Series : BARC External 05 Report type: Technical Report 06 Report No.: BARC/1999/E/043 07 Part No. or Volume No.: 08 Contract No.: 10 Title and subtitle: Redistribution of thermal x-ray radiation in cavities: view factor method and comparison with DSN calculations 11 Collation: 39 p., 9 figs. 13 Project No. : 20 Personal authors): 1) M.K. Srivastava 2) Vinod Kumar, S.V.G. Menon 21 Affiliation of authors): 1) Theoretical Physics Division, Bhabha Atomic Research Centre, Mumbai 2) Solid State and Spectroscopy Group, Bhabha Atomic Research Centre, Mumbai 22 Corporate authors): Bhabha Atomic Research Centre, Mumbai - 400 085 23 Originating unit: Theoretical Physics Division, BARC, Mumbai 24 Sponsors) Name: Department of Atomic Energy Type: Government Contd... (ii) -l- 30 Date of submission: December 1999 31 Publication/Issuedate: January 2000 40 Publisher/Distributor: Head, Library and Information Services Division, Bhabha Atomic Research Centre, Mumbai 42 Form of distribution: Hard copy 50 Language of text: English 51 Language ofsummary: English 52 No. -
Nuclear Energy in Everyday Life Nuclear Energy in Everyday Life
Nuclear Energy in Everyday Life Nuclear Energy in Everyday Life Understanding Radioactivity and Radiation in our Everyday Lives Radioactivity is part of our earth – it has existed all along. Naturally occurring radio- active materials are present in the earth’s crust, the floors and walls of our homes, schools, and offices and in the food we eat and drink. Our own bodies- muscles, bones and tissues, contain naturally occurring radioactive elements. Man has always been exposed to natural radiation arising from earth as well as from outside. Most people, upon hearing the word radioactivity, think only about some- thing harmful or even deadly; especially events such as the atomic bombs that were dropped on Hiroshima and Nagasaki in 1945, or the Chernobyl Disaster of 1986. However, upon understanding radiation, people will learn to appreciate that radia- tion has peaceful and beneficial applications to our everyday lives. What are atoms? Knowledge of atoms is essential to understanding the origins of radiation, and the impact it could have on the human body and the environment around us. All materi- als in the universe are composed of combination of basic substances called chemical elements. There are 92 different chemical elements in nature. The smallest particles, into which an element can be divided without losing its properties, are called atoms, which are unique to a particular element. An atom consists of two main parts namely a nu- cleus with a circling electron cloud. The nucleus consists of subatomic particles called protons and neutrons. Atoms vary in size from the simple hydro- gen atom, which has one proton and one electron, to large atoms such as uranium, which has 92 pro- tons, 92 electrons. -
Plant Lighting Basics and Applications
9/18/2012 Keywords Plant Lighting Basics and Light (radiation): electromagnetic wave that travels through space and exits as discrete Applications energy packets (photons) Each photon has its wavelength-specific energy level (E, in joule) Chieri Kubota The University of Arizona E = h·c / Tucson, AZ E: Energy per photon (joule per photon) h: Planck’s constant c: speed of light Greensys 2011, Greece : wavelength (meter) Wavelength (nm) 380 nm 780 nm Energy per photon [J]: E = h·c / Visible radiation (visible light) mole photons = 6.02 x 1023 photons Leaf photosynthesis UV Blue Green Red Far red Human eye response peaks at green range. Luminous intensity (footcandle or lux Photosynthetically Active Radiation ) does not work (PAR, 400-700 nm) for plant light environment. UV Blue Green Red Far red Plant biologically active radiation (300-800 nm) 1 9/18/2012 Chlorophyll a Phytochrome response Chlorophyll b UV Blue Green Red Far red Absorption spectra of isolated chlorophyll Absorptance 400 500 600 700 Wavelength (nm) Daily light integral (DLI or Daily Light Unit and Terminology PPF) Radiation Photons Visible light •Total amount of photosynthetically active “Base” unit Energy (J) Photons (mol) Luminous intensity (cd) radiation (400‐700 nm) received per sq Flux [total amount received Radiant flux Photon flux Luminous flux meter per day or emitted per time] (J s-1) or (W) (mol s-1) (lm) •Unit: mole per sq meter per day (mol m‐2 d‐1) Flux density [total amount Radiant flux density Photon flux (density) Illuminance, • Under optimal conditions, plant growth is received per area per time] (W m-2) (mol m-2 s-1) Luminous flux density highly correlated with DLI. -
Effects of Acute and Chronic Gamma Irradiation on the Cell Biology and Physiology of Rice Plants
plants Article Effects of Acute and Chronic Gamma Irradiation on the Cell Biology and Physiology of Rice Plants Hong-Il Choi 1,† , Sung Min Han 2,†, Yeong Deuk Jo 1 , Min Jeong Hong 1 , Sang Hoon Kim 1 and Jin-Baek Kim 1,* 1 Advanced Radiation Technology Institute, Korea Atomic Energy Research Institute, Jeongeup 56212, Korea; [email protected] (H.-I.C.); [email protected] (Y.D.J.); [email protected] (M.J.H.); [email protected] (S.H.K.) 2 Division of Ecological Safety, National Institute of Ecology, Seocheon 33657, Korea; [email protected] * Correspondence: [email protected]; Tel.: +82-63-570-3313 † Both authors contributed equally to this work. Abstract: The response to gamma irradiation varies among plant species and is affected by the total irradiation dose and dose rate. In this study, we examined the immediate and ensuing responses to acute and chronic gamma irradiation in rice (Oryza sativa L.). Rice plants at the tillering stage were exposed to gamma rays for 8 h (acute irradiation) or 10 days (chronic irradiation), with a total irradiation dose of 100, 200, or 300 Gy. Plants exposed to gamma irradiation were then analyzed for DNA damage, oxidative stress indicators including free radical content and lipid peroxidation, radical scavenging, and antioxidant activity. The results showed that all stress indices increased immediately after exposure to both acute and chronic irradiation in a dose-dependent manner, and acute irradiation had a greater effect on plants than chronic irradiation. The photosynthetic efficiency and growth of plants measured at 10, 20, and 30 days post-irradiation decreased in irradiated plants, Citation: Choi, H.-I.; Han, S.M.; Jo, Y.D.; Hong, M.J.; Kim, S.H.; Kim, J.-B. -
Chapter 3 the Mechanisms of Electromagnetic Emissions
BASICS OF RADIO ASTRONOMY Chapter 3 The Mechanisms of Electromagnetic Emissions Objectives: Upon completion of this chapter, you will be able to describe the difference between thermal and non-thermal radiation and give some examples of each. You will be able to distinguish between thermal and non-thermal radiation curves. You will be able to describe the significance of the 21-cm hydrogen line in radio astronomy. If the material in this chapter is unfamiliar to you, do not be discouraged if you don’t understand everything the first time through. Some of these concepts are a little complicated and few non- scientists have much awareness of them. However, having some familiarity with them will make your radio astronomy activities much more interesting and meaningful. What causes electromagnetic radiation to be emitted at different frequencies? Fortunately for us, these frequency differences, along with a few other properties we can observe, give us a lot of information about the source of the radiation, as well as the media through which it has traveled. Electromagnetic radiation is produced by either thermal mechanisms or non-thermal mechanisms. Examples of thermal radiation include • Continuous spectrum emissions related to the temperature of the object or material. • Specific frequency emissions from neutral hydrogen and other atoms and mol- ecules. Examples of non-thermal mechanisms include • Emissions due to synchrotron radiation. • Amplified emissions due to astrophysical masers. Thermal Radiation Did you know that any object that contains any heat energy at all emits radiation? When you’re camping, if you put a large rock in your campfire for a while, then pull it out, the rock will emit the energy it has absorbed as radiation, which you can feel as heat if you hold your hand a few inches away. -
Effects of Gamma-Irradiation of Seed Potatoes on Numbers of Stems and Tubers
Netherlands Journal of Agricultural Science 39 (1991) 81-90 Effects of gamma-irradiation of seed potatoes on numbers of stems and tubers A. J. HAVERKORT1, D. I. LANGERAK2 & M. VAN DE WAART1 1 Centre for Agrobiological Research (CABO-DLO), P.O. Box 14, NL 6700 AA Wagenin- gen, Netherlands 2 State Institute for Quality Control of Agricultural Products (RIKILT), P.O. Box 230, NL 6700 AE Wageningen, Netherlands Received 28 november 1990; accepted 8 February 1991 Abstract In field trials with the cultivars Bintje, Jaerla and Spunta, whose seed potatoes were treated with gamma-rays from a ^Co source with doses varying from 0.5 to 27 Gy, tuber yield, har vest index, and number of stems and tubers were determined. A dose of 3 Gy increased the number of tubers by 30 % in Spunta in two out of three trials and by 17 % in one trial in Jaer la, but it did not increase number of tubers in Bintje. Doses of 9 or 10 Gy did not influence the number of tubers nor stems, and decreased harvest index. A dose of 27 Gy yielded off-type plants with reduced yield and number of tubers. Gamma-radiation affected the growth of the apex of the sprout allowing lateral buds or divisions of the affected apex to develop into stems. To achieve larger numbers of tuber-bearing stems, tubers should preferably be irra diated at the start of sprout growth, about 5 months before planting. Keywords: harvest index, gamma irradiation, seed potatoes Introduction Effects of different doses of gamma-rays on potato tubers have been studied exten sively, especially in the 1960s. -
Industrial Applications of Electron Accelerators
Industrial applications of electron accelerators M.R. Cleland Ion Beam Applications, Edgewood, NY 11717, USA Abstract This paper addresses the industrial applications of electron accelerators for modifying the physical, chemical or biological properties of materials and commercial products by treatment with ionizing radiation. Many beneficial effects can be obtained with these methods, which are known as radiation processing. The earliest practical applications occurred during the 1950s, and the business of radiation processing has been expanding since that time. The most prevalent applications are the modification of many different plastic and rubber products and the sterilization of single-use medical devices. Emerging applications are the pasteurization and preservation of foods and the treatment of toxic industrial wastes. Industrial accelerators can now provide electron energies greater than 10 MeV and average beam powers as high as 700 kW. The availability of high-energy, high-power electron beams is stimulating interest in the use of X-rays (bremsstrahlung) as an alternative to gamma rays from radioactive nuclides. 1 Introduction Radiation processing can be defined as the treatment of materials and products with radiation or ionizing energy to change their physical, chemical or biological characteristics, to increase their usefulness and value, or to reduce their impact on the environment. Accelerated electrons, X-rays (bremsstrahlung) emitted by energetic electrons, and gamma rays emitted by radioactive nuclides are suitable energy sources. These are all capable of ejecting atomic electrons, which can then ionize other atoms in a cascade of collisions. So they can produce similar molecular effects. The choice of energy source is usually based on practical considerations, such as absorbed dose, dose uniformity (max/min) ratio, material thickness, density and configuration, processing rate, capital and operating costs. -
Influence of Radiation Damage on Xenon Diffusion in Silicon Carbide
Influence of radiation damage on xenon diffusion in silicon carbide E. Friedland*a, K. Gärtnerb, T.T. Hlatshwayoa, N.G. van der Berga, T.T. Thabethea a Physics Department, University of Pretoria, Pretoria, South Africa b Institut für Festkörperphysik, Friedrich-Schiller-Universität, Jena, Germany Keywords silicon carbide, diffusion, radiation damage *Corresponding author. E mail: [email protected], Phone: +27-12-4202453, Fax: +27-12-3625288 Diffusion of xenon in poly and single crystalline silicon carbide and the possible influence of radiation damage on it are investigated. For this purpose 360 keV xenon ions were implanted in commercial 6H-SiC and CVD-SiC wafers at room temperature, 350 °C and 600 °C. Width broadening of the implantation pro- files and xenon retention during isochronal and isothermal annealing up to temperatures of 1500 °C was de- termined by RBS-analysis, whilst in the case of 6H-SiC damage profiles were simultaneously obtained by a- particle channelling. No diffusion or xenon loss was detected in the initially amorphized and eventually re- crystallized surface layer of cold implanted 6H-SiC during annealing up to 1200 °C. Above that temperature serious erosion of the implanted surface occurred, which made any analysis impossible. No diffusion or xen- on loss is detected in the hot implanted 6H-SiC samples during annealing up to 1400 °C. Radiation damage dependent grain boundary diffusion is observed at 1300 °C in CVD-SiC. 1 Introduction Modern high-temperature nuclear reactors (HTR’s) commonly use fuel elements containing triple isotropic cladded (TRISO) fuel particles. These are fuel kernels surrounded by four successive lay- ers of low-density pyrolitic carbon, high-density pyrolitic carbon, silicon carbide and high-density pyrolitic carbon, with silicon carbide being the main barrier to prevent the release of fission prod- ucts. -
Applied Spectroscopy Spectroscopic Nomenclature
Applied Spectroscopy Spectroscopic Nomenclature Absorbance, A Negative logarithm to the base 10 of the transmittance: A = –log10(T). (Not used: absorbancy, extinction, or optical density). (See Note 3). Absorptance, α Ratio of the radiant power absorbed by the sample to the incident radiant power; approximately equal to (1 – T). (See Notes 2 and 3). Absorption The absorption of electromagnetic radiation when light is transmitted through a medium; hence ‘‘absorption spectrum’’ or ‘‘absorption band’’. (Not used: ‘‘absorbance mode’’ or ‘‘absorbance band’’ or ‘‘absorbance spectrum’’ unless the ordinate axis of the spectrum is Absorbance.) (See Note 3). Absorption index, k See imaginary refractive index. Absorptivity, α Internal absorbance divided by the product of sample path length, ℓ , and mass concentration, ρ , of the absorbing material. A / α = i ρℓ SI unit: m2 kg–1. Common unit: cm2 g–1; L g–1 cm–1. (Not used: absorbancy index, extinction coefficient, or specific extinction.) Attenuated total reflection, ATR A sampling technique in which the evanescent wave of a beam that has been internally reflected from the internal surface of a material of high refractive index at an angle greater than the critical angle is absorbed by a sample that is held very close to the surface. (See Note 3.) Attenuation The loss of electromagnetic radiation caused by both absorption and scattering. Beer–Lambert law Absorptivity of a substance is constant with respect to changes in path length and concentration of the absorber. Often called Beer’s law when only changes in concentration are of interest. Brewster’s angle, θB The angle of incidence at which the reflection of p-polarized radiation is zero. -
High Altitude Nuclear Detonations (HAND) Against Low Earth Orbit Satellites ("HALEOS")
High Altitude Nuclear Detonations (HAND) Against Low Earth Orbit Satellites ("HALEOS") DTRA Advanced Systems and Concepts Office April 2001 1 3/23/01 SPONSOR: Defense Threat Reduction Agency - Dr. Jay Davis, Director Advanced Systems and Concepts Office - Dr. Randall S. Murch, Director BACKGROUND: The Defense Threat Reduction Agency (DTRA) was founded in 1998 to integrate and focus the capabilities of the Department of Defense (DoD) that address the weapons of mass destruction (WMD) threat. To assist the Agency in its primary mission, the Advanced Systems and Concepts Office (ASCO) develops and maintains and evolving analytical vision of necessary and sufficient capabilities to protect United States and Allied forces and citizens from WMD attack. ASCO is also charged by DoD and by the U.S. Government generally to identify gaps in these capabilities and initiate programs to fill them. It also provides support to the Threat Reduction Advisory Committee (TRAC), and its Panels, with timely, high quality research. SUPERVISING PROJECT OFFICER: Dr. John Parmentola, Chief, Advanced Operations and Systems Division, ASCO, DTRA, (703)-767-5705. The publication of this document does not indicate endorsement by the Department of Defense, nor should the contents be construed as reflecting the official position of the sponsoring agency. 1 Study Participants • DTRA/AS • RAND – John Parmentola – Peter Wilson – Thomas Killion – Roger Molander – William Durch – David Mussington – Terry Heuring – Richard Mesic – James Bonomo • DTRA/TD – Lewis Cohn • Logicon RDA – Les Palkuti – Glenn Kweder – Thomas Kennedy – Rob Mahoney – Kenneth Schwartz – Al Costantine – Balram Prasad • Mission Research Corp. – William White 2 3/23/01 2 Focus of This Briefing • Vulnerability of commercial and government-owned, unclassified satellite constellations in low earth orbit (LEO) to the effects of a high-altitude nuclear explosion. -
Bio-9 a Comparison of Y-Irradiation and Microwave Treatments on the Lipids and Microbiological Pattern of Beef Liver
Seventh Conference of Nuclear Sciences & Applications 6-10 February 2000, Cairo, Egypt Bio-9 A comparison of y-irradiation and microwave treatments on the lipids and microbiological pattern of beef liver Farag, R. S .*, Z. Y. Daw2, Farag , S.A 3 and Safaa A. E. ABD El-Wahab3. / Biochemistry Department, Faculty of Agriculture, Cairo University, Giza - Egypt. 2 Microbiology Department. Faculty of Agriculture. Cairo University, Giza - Egypt. 3 Food irradiation Department, National Center for Radiation Research and Technology, Cairo - Egypt. ABSTRACT EG0100123 The effects of y-irradiation treatments (0, 2.5, 5 and, 10 kGy) and microwaves generated from an oven at low and defrost settings for 0.5 , 1 and 2 min on the chemical composition and microbiological aspects of beef liver samples were studied . The chemical and microbiological analyses were performed on the non-treated and treated beef liver immediately after treatments and during frozen storage (-18°C) for 3 months. The chemical analyses of beef liver Hpids showed that acid, peroxide and TBA(Thiobarbituric acid ) values were slightly increased after irradiation treatments and also during frozen storage (-18°C). On the contrary, iodine value of the treated beef liver was decreased. Irradiation treatments remarkably reduced the total bacterial counts in beef liver. The percent reduction of bacterial load for beef liver exposed to microwaves generated from an oven at defrost mode for 2 min and after 3 months at - 18°C was 62% . The bacterial load for beef liver exposed to y-irradiation at 10 kGy after 3 months at - 18°C was decreased by 98%. Hence, y-irradiation treatment was far better than microwave treatment for inhibiting the multiplication of the associated microorganisms with beef liver.