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FT/P3-20 Physics and Engineering Basis of Multi-Functional Compact Tokamak Reactor Concept R.M.O
FT/P3-20 Physics and Engineering Basis of Multi-functional Compact Tokamak Reactor Concept R.M.O. Galvão1, G.O. Ludwig2, E. Del Bosco2, M.C.R. Andrade2, Jiangang Li3, Yuanxi Wan3 Yican Wu3, B. McNamara4, P. Edmonds, M. Gryaznevich5, R. Khairutdinov6, V. Lukash6, A. Danilov7, A. Dnestrovskij7 1CBPF/IFUSP, Rio de Janeiro, Brazil, 2Associated Plasma Laboratory, National Space Research Institute, São José dos Campos, SP, Brazil, 3Institute of Plasma Physics, CAS, Hefei, 230031, P.R. China, 4Leabrook Computing, Bournemouth, UK, 5EURATOM/UKAEA Fusion Association, Culham Science Centre, Abingdon, UK, 6TRINITI, Troitsk, RF, 7RRC “Kurchatov Institute”, Moscow, RF [email protected] Abstract An important milestone on the Fast Track path to Fusion Power is to demonstrate reliable commercial application of Fusion as soon as possible. Many applications of fusion, other than electricity production, have already been studied in some depth for ITER class facilities. We show that these applications might be usefully realized on a small scale, in a Multi-Functional Compact Tokamak Reactor based on a Spherical Tokamak with similar size, but higher fields and currents than the present experiments NSTX and MAST, where performance has already exceeded expectations. The small power outputs, 20-40MW, permit existing materials and technologies to be used. The analysis of the performance of the compact reactor is based on the solution of the global power balance using empirical scaling laws considering requirements for the minimum necessary fusion power (which is determined by the optimized efficiency of the blanket design), positive power gain and constraints on the wall load. In addition, ASTRA and DINA simulations have been performed for the range of the design parameters. -
小型飛翔体/海外 [Format 2] Technical Catalog Category
小型飛翔体/海外 [Format 2] Technical Catalog Category Airborne contamination sensor Title Depth Evaluation of Entrained Products (DEEP) Proposed by Create Technologies Ltd & Costain Group PLC 1.DEEP is a sensor analysis software for analysing contamination. DEEP can distinguish between surface contamination and internal / absorbed contamination. The software measures contamination depth by analysing distortions in the gamma spectrum. The method can be applied to data gathered using any spectrometer. Because DEEP provides a means of discriminating surface contamination from other radiation sources, DEEP can be used to provide an estimate of surface contamination without physical sampling. DEEP is a real-time method which enables the user to generate a large number of rapid contamination assessments- this data is complementary to physical samples, providing a sound basis for extrapolation from point samples. It also helps identify anomalies enabling targeted sampling startegies. DEEP is compatible with small airborne spectrometer/ processor combinations, such as that proposed by the ARM-U project – please refer to the ARM-U proposal for more details of the air vehicle. Figure 1: DEEP system core components are small, light, low power and can be integrated via USB, serial or Ethernet interfaces. 小型飛翔体/海外 Figure 2: DEEP prototype software 2.Past experience (plants in Japan, overseas plant, applications in other industries, etc) Create technologies is a specialist R&D firm with a focus on imaging and sensing in the nuclear industry. Createc has developed and delivered several novel nuclear technologies, including the N-Visage gamma camera system. Costainis a leading UK construction and civil engineering firm with almost 150 years of history. -
4. Particle Generators/Accelerators
Joint innovative training and teaching/ learning program in enhancing development and transfer knowledge of application of ionizing radiation in materials processing 4. Particle Generators/Accelerators Diana Adlienė Department of Physics Kaunas University of Technolog y Joint innovative training and teaching/ learning program in enhancing development and transfer knowledge of application of ionizing radiation in materials processing This project has been funded with support from the European Commission. This publication reflects the views only of the author. Polish National Agency and the Commission cannot be held responsible for any use which may be made of the information contained therein. Date: Oct. 2017 DISCLAIMER This presentation contains some information addapted from open access education and training materials provided by IAEA TABLE OF CONTENTS 1. Introduction 2. X-ray machines 3. Particle generators/accelerators 4. Types of industrial irradiators The best accelerator in the universe… INTRODUCTION • Naturally occurring radioactive sources: – Up to 5 MeV Alpha’s (helium nuclei) – Up to 3 MeV Beta particles (electrons) • Natural sources are difficult to maintain, their applications are limited: – Chemical processing: purity, messy, and expensive; – Low intensity; – Poor geometry; – Uncontrolled energies, usually very broad Artificial sources (beams) are requested! INTRODUCTION • Beams of accelerated particles can be used to produce beams of secondary particles: Photons (x-rays, gamma-rays, visible light) are generated from beams -
Depleted Uranium Technical Brief
Disclaimer - For assistance accessing this document or additional information,please contact [email protected]. Depleted Uranium Technical Brief United States Office of Air and Radiation EPA-402-R-06-011 Environmental Protection Agency Washington, DC 20460 December 2006 Depleted Uranium Technical Brief EPA 402-R-06-011 December 2006 Project Officer Brian Littleton U.S. Environmental Protection Agency Office of Radiation and Indoor Air Radiation Protection Division ii iii FOREWARD The Depleted Uranium Technical Brief is designed to convey available information and knowledge about depleted uranium to EPA Remedial Project Managers, On-Scene Coordinators, contractors, and other Agency managers involved with the remediation of sites contaminated with this material. It addresses relative questions regarding the chemical and radiological health concerns involved with depleted uranium in the environment. This technical brief was developed to address the common misconception that depleted uranium represents only a radiological health hazard. It provides accepted data and references to additional sources for both the radiological and chemical characteristics, health risk as well as references for both the monitoring and measurement and applicable treatment techniques for depleted uranium. Please Note: This document has been changed from the original publication dated December 2006. This version corrects references in Appendix 1 that improperly identified the content of Appendix 3 and Appendix 4. The document also clarifies the content of Appendix 4. iv Acknowledgments This technical bulletin is based, in part, on an engineering bulletin that was prepared by the U.S. Environmental Protection Agency, Office of Radiation and Indoor Air (ORIA), with the assistance of Trinity Engineering Associates, Inc. -
Radiation Quick Reference Guide Recommend Contacting Your State Fusion Center
Domestic Nuclear Detection Office If you encounter something suspicious follow your specific local protocols. Radiation Quick Reference Guide Recommend contacting your state fusion center. DNDO is available 24/7 to assist at 1-877-DNDO-JAC / 1-877-363-6522 JAC Information Line 202-254-7179 Email: [email protected] Nuclear Concerns/ Threats 1. Nuclear Weapon - a device that releases nuclear energy in an ex- Isotopes of Concern for use in RDDs - with common uses plosive manner. Uses Highly Enriched Uranium (HEU) and/or 1. Cobalt-60 – cancer treatment, level/ Plutonium. density gauge, teletherapy, radiography, 2. Improvised Nuclear Device (IND) - a nuclear weapon fabricated food sterilization/irradiation, by a terrorist organization or rogue nation. brachytherapy 2. Iridium-192 – Radiography/non- destructive testing, flaw detection, brachy- therapy “cancer seed”, skin cancer Cobalt 60 sources Uranium “superficial” brachytherapy Plutonium 3. Uranium a. Uranium exists naturally in the earth’s crust. Of the different “isotopes” of uranium, U-235 is the one required to produce a Iridium sentinel and nuclear weapon. gamma camera b. Natural uranium contains a small amount of U-235 (<1%) which Cesium Seeds must be separated in complex extraction processes to create HEU. The predominant uranium isotope is U-238. 3. Cesium-137 - Gauge/level gauge, industrial radiography, brachyther- c. Highly Enriched Uranium (HEU) refers to uranium usable in weap- apy/teletherapy, well logging/density gauges ons due to its enrichment in U-235. 4. Strontium-90 – Radioisotope thermoelectric generator (RTG), fis- d. Approximately 25 kg of HEU is required for a nuclear weapon. sion product, industrial gauges, medical treatment e. -
Installation of the Cyclotron Based Clinical Neutron Therapy System in Seattle
Proceedings of the Tenth International Conference on Cyclotrons and their Applications, East Lansing, Michigan, USA INSTALLATION OF THE CYCLOTRON BASED CLINICAL NEUTRON THERAPY SYSTEM IN SEATTLE R. Risler, J. Eenmaa, J. Jacky, I. Kalet, and P. Wootton Medical Radiation Physics RC-08, University of Washington, Seattle ~ 98195, USA S. Lindbaeck Instrument AB Scanditronix, Uppsala, Sweden Sumnary radiation areas is via sliding shielding doors rather than a maze, mai nl y to save space. For the same reason A cyclotron facility has been built for cancer a single door is used to alternately close one or the treatment with fast neutrons. 50.5 MeV protons from a other therapy room. All power supplies and the control conventional, positive ion cyclotron are used to b0m computer are located on the second floor, above the bard a semi-thick Beryllium target located 150 am from maintenance area. The cooler room contains a heat the treatment site. Two treatment rooms are available, exchanger and other refrigeration equipment. Not shown one with a fixed horizontal beam and one with an iso in the diagram is the cooling tower located in another centric gantry capable of 360 degree rotation. In part of the building. Also not shown is the hot lab addition 33 51 MeV protons and 16.5 - 25.5 MeV now under construction an an area adjacent to the deuterons are generated for isotope production inside cyclotron vault. It will be used to process radio the cyclotron vault. The control computer is also used isotopes produced at a target station in the vault. to record and verify treatment parameters for indi vidual patients and to set up and monitor the actual radiation treatment. -
22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons
22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons to 2 MeV by Leslie Dewan Submitted to the Department of Nuclear Science and Engineering in Partial Fulfillment of the Requirements for the Degree of Bachelor of Science in Nuclear Science and Engineering at the Massachusetts Institute of Technology June 2007 © 2007 Leslie Dewan All rights reserved The author hereby grants to MIT permission to reproduce and to distribute publicly paper and electronic copies of this thesis document in whole or in part in any medium now known or hereafter created. Signature of Author: Leslie Dewan Department of Nuclear Science and Engineering May 16, 2007 Certified by: David G. Cory Professor of Nuclear Science and Engineering Thesis Supervisor Accepted by: David G. Cory Professor of Nuclear Science and Engineering Chairman, NSE Committee for Undergraduate Students Leslie Dewan 1 of 23 5/16/07 22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons to 2 MeV by Leslie Dewan Submitted to the Department of Nuclear Science and Engineering on May 16, 2007 in Partial Fulfillment of the Requirements for the Degree of Bachelor of Science in Nuclear Science and Engineering ABSTRACT This thesis describes the design and construction of a cyclotron capable of accelerating protons to 2 MeV. A cyclotron is a charged particle accelerator that uses a magnetic field to confine particles to a spiral flight path in a vacuum chamber. An applied electrical field accelerates these particles to high energies, typically on the order of mega-electron volts. -
Disposal of Radioisotope Thermoelectric Generators; Problems, and How to Solve Them
DISPOSAL OF RADIOISOTOPE THERMOELECTRIC GENERATORS; PROBLEMS, AND HOW TO SOLVE THEM N.R. Kuzelev, Ye.N. Kroschkin, A.G. Kataschov - FSUE “VNIITFA”. 1. The work carried out at “VNIITFA” in 2007 The following work for disposal of RTGs was carried out at “VNIITFA” in 2007: USA - For the money allocated by the US we completed the work on developing of the database of all the RTGs located on the territory of the Russian Federation. 21 RTGs were tested in the Far East and in Kamchatka. Besides, the US coordinated the work financed by the Canadian side on decommissioning of 10 RTGs from the Tiksi Bay, as well as installation of 9 alternative power sources in the Strait of Yugorsky Schar. Canada - in accordance with the Executive Agreement with the Ministry of Foreign Affairs and International Trade of Canada 17 transportation containers for transporting RHSes were fabricated, as well as 16 sets of secure containers for transporting RTGs. The above equipment is currently being used to transport RTGs and RHSes for disposal. Norway - removal of RTGs from the coast of the Barents Sea continued with the technical assistance of Norway. Totally 21 RTGs were removed and disassembled due to the money of Norway. Currently there are no RTGs on the Kola Peninsula. Russia - for the money of the Russian Federation the work was carried out to eliminate radiation accident with the RTG at Navarin lighthouse, as well as 3 RTGs from the Baltic region were disposed of with a certain preliminary work. Inspection of 10 RTGs was carried out in Yakutia (Peleduy). -
Cyclotrons: Old but Still New
Cyclotrons: Old but Still New The history of accelerators is a history of inventions William A. Barletta Director, US Particle Accelerator School Dept. of Physics, MIT Economics Faculty, University of Ljubljana US Particle Accelerator School ~ 650 cyclotrons operating round the world Radioisotope production >$600M annually Proton beam radiation therapy ~30 machines Nuclear physics research Nuclear structure, unstable isotopes,etc High-energy physics research? DAEδALUS Cyclotrons are big business US Particle Accelerator School Cyclotrons start with the ion linac (Wiederoe) Vrf Vrf Phase shift between tubes is 180o As the ions increase their velocity, drift tubes must get longer 1 v 1 "c 1 Ldrift = = = "# rf 2 f rf 2 f rf 2 Etot = Ngap•Vrf ==> High energy implies large size US Particle Accelerator School ! To make it smaller, Let’s curl up the Wiederoe linac… Bend the drift tubes Connect equipotentials Eliminate excess Cu Supply magnetic field to bend beam 1 2# mc $ 2# mc " rev = = % = const. frf eZion B eZion B Orbits are isochronous, independent of energy ! US Particle Accelerator School … and we have Lawrence’s* cyclotron The electrodes are excited at a fixed frequency (rf-voltage source) Particles remain in resonance throughout acceleration A new bunch can be accelerated on every rf-voltage peak: ===> “continuous-wave (cw) operation” Lawrence, E.O. and Sloan, D.: Proc. Nat. Ac. Sc., 17, 64 (1931) Lawrence, E.O. & Livingstone M.S.: Phys. Rev 37, 1707 (1931). * The first cyclotron patent (German) was filed in 1929 by Leó Szilard but never published in a journal US Particle Accelerator School Synchronism only requires that τrev = N/frf “Isochronous” particles take the same revolution time for each turn. -
CURIUM Element Symbol: Cm Atomic Number: 96
CURIUM Element Symbol: Cm Atomic Number: 96 An initiative of IYC 2011 brought to you by the RACI ROBYN SILK www.raci.org.au CURIUM Element symbol: Cm Atomic number: 96 Curium is a radioactive metallic element of the actinide series, and named after Marie Skłodowska-Curie and her husband Pierre, who are noted for the discovery of Radium. Curium was the first element to be named after a historical person. Curium is a synthetic chemical element, first synthesized in 1944 by Glenn T. Seaborg, Ralph A. James, and Albert Ghiorso at the University of California, Berkeley, and then formally identified by the same research tea at the wartime Metallurgical Laboratory (now Argonne National Laboratory) at the University of Chicago. The discovery of Curium was closely related to the Manhattan Project, and thus results were kept confidential until after the end of World War II. Seaborg finally announced the discovery of Curium (and Americium) in November 1945 on ‘The Quiz Kids!’, a children’s radio show, five days before an official presentation at an American Chemical Society meeting. The first radioactive isotope of Curium discovered was Curium-242, which was made by bombarding alpha particles onto a Plutonium-239 target in a 60-inch cyclotron (University of California, Berkeley). Nineteen radioactive isotopes of Curium have now been characterized, ranging in atomic mass from 233 to 252. The most stable radioactive isotopes are Curium- 247 with a half-life of 15.6 million years, Curium-248 (half-life 340,000 years), Curium-250 (half-life of 9000 years), and Curium-245 (half-life of 8500 years). -
Cyclotron Basics
Unit 10 - Lectures 14 Cyclotron Basics MIT 8.277/6.808 Intro to Particle Accelerators Timothy A. Antaya Principal Investigator MIT Plasma Science and Fusion Center [email protected] / (617) 253-8155 1 Outline Introduce an important class of circular particle accelerators: Cyclotrons and Synchrocyclotrons Identify the key characteristics and performance of each type of cyclotron and discuss their primary applications Discuss the current status of an advance in both the science and engineering of these accelerators, including operation at high magnetic field Overall aim: reach a point where it will be possible for to work a practical exercise in which you will determine the properties of a prototype high field cyclotron design (next lecture) [email protected] / (617) 253-8155 2 Motion in a magnetic field [email protected] / (617) 253-8155 3 Magnetic forces are perpendicular to the B field and the motion [email protected] / (617) 253-8155 4 Sideways force must also be Centripedal [email protected] / (617) 253-8155 5 Governing Relation in Cyclotrons A charge q, in a uniform magnetic field B at radius r, and having tangential velocity v, sees a centripetal force at right angles to the direction of motion: mv2 r rˆ = qvr ! B r The angular frequency of rotation seems to be independent of velocity: ! = qB / m [email protected] / (617) 253-8155 6 Building an accelerator using cyclotron resonance condition A flat pole H-magnet electromagnet is sufficient to generate require magnetic field Synchronized electric fields can be used to raise -
Electrostatic Particle Accelerators the Cyclotron Linear Particle Accelerators the Synchrotron +
Uses: Mass Spectrometry Uses Overview Uses: Hadron Therapy This is a technique in analytical chemistry. Ionising particles such as protons are fired into the It allows the identification of chemicals by ionising them body. They are aimed at cancerous tissue. and measuring the mass to charge ratio of each ion type Most methods like this irradiate the surrounding tissue too, against relative abundance. but protons release most of their energy at the end of their It also allows the relative atomic mass of different elements travel. (see graphs) be measured by comparing the relative abundance of the This allows the cancer cells to be targeted more precisely, with ions of different isotopes of the element. less damage to surrounding tissue. An example mass spectrum is shown below: Linear Particle Accelerators Electrostatic Particle Accelerators These are still in a straight line, but now the voltage is no longer static - it is oscillating. An electrostatic voltageis provided at one end of a vacuum tube. This means the voltage is changing - so if it were a magnet, it would be first positive, then This is like the charge on a magnet. negative. At the other end of the tube, there are particles Like the electrostatic accelerator, a charged particle is attracted to it as the charges are opposite, but just with the opposite charge. as the particle goes past the voltage changes, and the charge of the plate swaps (so it is now the same charge Like north and south poles on a magnet, the opposite charges as the particle). attract and the particle is pulled towards the voltage.