FUSION Quarterly News & Views on the Progress in Fusion Research
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A European Success Story the Joint European Torus
EFDA JET JETJETJET LEAD ING DEVICE FOR FUSION STUDIES HOLDER OF THE WORLD RECORD OF FUSION POWER PRODUCTION EXPERIMENTS STRONGLY FOCUSSED ON THE PREPARATION FOR ITER EXPERIMENTAL DEVICE USED UNDER THE EUROPEAN FUSION DEVELOPEMENT AGREEMENT THE JOINT EUROPEAN TORUS A EUROPEAN SUCCESS STORY EFDA Fusion: the Energy of the Sun If the temperature of a gas is raised above 10,000 °C virtually all of the atoms become ionised and electrons separate from their nuclei. The result is a complete mix of electrons and ions with the sum of all charges being very close to zero as only small charge imbalance is allowed. Thus, the ionised gas remains almost neutral throughout. This constitutes a fourth state of matter called plasma, with a wide range of unique features. D Deuterium 3He Helium 3 The sun, and similar stars, are sphe- Fusion D T Tritium res of plasma composed mainly of Li Lithium hydrogen. The high temperature, 4He Helium 4 3He Energy U Uranium around 15 million °C, is necessary released for the pressure of the plasma to in Fusion T balance the inward gravitational for- ces. Under these conditions it is pos- Li Fission sible for hydrogen nuclei to fuse together and release energy. Nuclear binding energy In a terrestrial system the aim is to 4He U produce the ‘easiest’ fusion reaction Energy released using deuterium and tritium. Even in fission then the rate of fusion reactions becomes large enough only at high JG97.362/4c Atomic mass particle energy. Therefore, when the Dn required nuclear reactions result from the thermal motions of the nuclei, so-called thermonuclear fusion, it is necessary to achieve u • extremely high temperatures, of at least 100 million °C. -
2019 EPS PPD Report
Report from the EPS Plasma Physics Division Board, Summer 2019 Board meetings The Board met twice in 2018, on 1st July in Prague (CZ) and on 13th December at Culham (UK). Operation of the Division Richard Dendy (Culham Centre for Fusion Energy and Warwick University, UK) continues as Chair 2016-2020 of the Division, and Kristel Crombé (ERM/KMS and Ghent University, Belgium) continues as Secretary. The Board members leading the arrangements for the competitions for the 2018 EPS-PPD Prizes were: Alfvén, John Kirk (Max Planck Institute for Nuclear Physics, Germany); Innovation, Holger Kersten (Kiel University, Germany) and Eva Kovačević (Orléans University, France); PhD Research Award, Carlos Silva (Instituto Superior Técnico, Portugal). Further information is available at http://plasma.ciemat.es/eps/board/. Prague EPS Plasma Physics Conference 2018 (https://eps2018.eli-beams.eu/en/) The successful 45th annual EPS Plasma Physics Conference took place at the Žofín Palace in Prague from 2nd to 6th July 2018, hosted by a consortium of Czech plasma research organisations. The Local Organising Committee was ably chaired by Stefan Weber (ELI-Beamlines), who is also an EPS-PPD Board member. The Programme Committee was ably chaired by Stefano Coda (CH) and comprised: •MCF: M. Mantsinen (ES – sub-chair), T. Eich (DE), G. Ericsson (SE), L. Frassinetti (SE), G. Huijsmans (ITER), R. König (DE), J. Mailloux (UK), P. Piovesan (IT), R. Zagorski (PL) •BPIF: C. Michaut (FR – sub-chair), O. Klimo (CZ), M. Nakatsutsumi (XFEL), A. Ravasio (FR), S. Kar (UK), R. Scott (UK) •BSAP: G. Lapenta (BE – sub-chair), M.E. Dieckmann (SE), E. -
Fusion: the Way Ahead
Fusion: the way ahead Feature: Physics World March 2006 pages 20 - 26 The recent decision to build the world's largest fusion experiment - ITER - in France has thrown down the gauntlet to fusion researchers worldwide. Richard Pitts, Richard Buttery and Simon Pinches describe how the Joint European Torus in the UK is playing a key role in ensuring ITER will demonstrate the reality of fusion power At a Glance: Fusion power • Fusion is the process whereby two light nuclei bind to form a heavier nucleus with the release of energy • Harnessing fusion on Earth via deuterium and tritium reactions would lead to an environmentally friendly and almost limitless energy source • One promising route to fusion power is to magnetically confine a hot, dense plasma inside a doughnut-shaped device called a tokamak • The JET tokamak provides a vital testing ground for understanding the physics and technologies necessary for an eventual fusion reactor • ITER is due to power up in 2016 and will be the next step towards a demonstration fusion power plant, which could be operational by 2035 By 2025 the Earth's population is predicted to reach eight billion. By the turn of the next century it could be as many as 12 billion. Even if the industrialized nations find a way to reduce their energy consumption, this unprecedented increase in population - coupled with rising prosperity in the developing world - will place huge demands on global energy supplies. As our primary sources of energy - fossil fuels - begin to run out, and burning them causes increasing environmental concerns, the human race faces the challenge of finding new energy sources. -
DISTRIBUTION of THIS DOCUMENT IS UNLIMITED Temperatures in the Range 5-10 Kev Are Still Needed, but the Lawson Number Can Be Reduced to the Low 10 Cm Sec Range
TFTR and Other Large Tokamaks Plasma Physics Laboratory, Princeton University Princeton, New Jersey 08544 H.P. Furth CONF-8604223—1 DE86 012761 Introduction The near-term goal of fusion research is to produce deuterium-tritium plasmas with temperatures above 10 keV and Lawson numbers nTE above 10 cm sec. As indicated in Fig. 1, experiments entering this parameter range will be able to satisfy Lawson's break-even criterion, where the fusion power output equals the required plasma-heating-power input (Q = 1 ). The ultimate reactor goal is to reach equilibrium-burn conditions, where the energetic alpha particles generated by the D-T reaction are sufficient to maintain the plasma temperature against all heat losses (Q = °°). At the outset of the international controlled-fusion research effort in the 19 50's, Lawson's goal seemed intimidatingly remote from experimental capabilities. During the following ten years, substantial scientific progress was made, but the rate of advance in the Lawson diagram was not such as to inspire confidence that the fusion program would reach fruition within the lifetime of its pioneers. The notable success of the Kurchatov Institute's T-3 tokamak during 1968-69 brightened the outlook considerably. The tokamak configuration was recognized as a cost-effective experimental tool and has permitted steady progress during subsequent decades. World-wide recognition of the favorable experimental opportunity for entry into the reactor plasma regime led to the initiation, in the mid-1970's, of four large new tokamak projects (Table I). Plans for the Joint European Torus (JET) were defined in 1971-73: th_ very large plasma size and high current of the JET plasma offered a potential for exceeding the Lawson break- even criterion and possibly evan reaching ignition in D-T plasmas. -
Corrosion Issues in Fusion Reactors
Corrosion Issues in Fusion Reactors Digby D. Macdonald1 and George R. Engelhardt2 1Department of Nuclear Engineering University of California at Berkeley Berkeley, CA 94720 2OLI Systems, Inc. 240 Cedar Knolls Rd Cedar Knolls, NJ 07927 WCO Forum Corrosion 2020 Houston, TX, USA Background • Nuclear fusion is the process of fusing the light elements (primarily 1 2 3 the isotopes of hydrogen, H1, D1, T1. • Fusion results in a loss of mass, which is converted into energy, E = Δm.c2. • Process that occurs in the sun and stars in nuclear synthesis. Minimum temperature for D + T is 10 keV = 300,000,000 oC equivalent. • First demonstrated on earth in 1950s through thermonuclear weapons. • Almost a limitless source of clean energy if it can be made to work. • First controlled fusion demonstrated at JET in Oxford, UK, Q =0.75. • First technology demonstration, ITER (‘the way”), being constructed at Cadarache, France. Q > 10. Thermonuclear Reactions Reaction Reaction Equation Initial Mass (u) Mass Change (u) % Mass Change 2 2 3 1 -3 D-D D1 + D1 → He2 + n0 4.027106424 -2.44152x10 0.06062 2 2 3 1 -3 D-D D1 + D1 → H1 + p1 4.027106424 -3.780754x10 0.09388 2 3 4 1 D-T D1 + T1 → He2 + n0 5.029602412 -0.019427508 0.3863 e--p+ e- + p+ → 2hν 1.8219x10-31 -1.8219x10-31 100 Must overcome Coulombic repulsion of nuclei in the plasma Preferred Reaction • The easiest reaction to achieve 2 3 4 1 is: D1 + T1 → He2 + n0 because it has the lowest ignition temperature (10 keV). -
June 2018 Fusion in Europe
FUSION IN EUROPE NEWS & VIEWS ON THE PROGRESS OF FUSION RESEARCH “Let us face it: TO DTT OR NOT TO DTT there is no VACUUM – HOW NOTHING REALLY planet B!” MATTERS NOW IS THE TIME TO BE AT JET 2 2018 Fusion Writers … wanted! … and Artists This could be you Fusion in Europe is call- ing for aspiring writers and gifted artists! Introduce yourself to an international audience! Catch one of our topics and turn it into your own! • The future powered by fusion energy • Fusion science and industrial reality • Fusion - a melting pot of different sciences • Fusion drives innovation Find the entire list here: tinyurl.com/ybd4omz7 Your application should include a short CV and a motivational letter. Please apply here: tinyurl.com/ybd4omz7 EUROfusion | Communications Team | Anne Purschwitz (”Fusion in Europe“ Editor) Boltzmannstr. 2 | 85748Application Garching | +49 89 deadline: 3299 4128 | [email protected] 25 June 2018 | Editorial | EUROfusion | “It is the best time to be at JET right now” says a passionate Eva Belo nohy. The member of JET’s Exploitation Unit has recently organised a very suc- cessful workshop. It was aimed to ‘refresh’ the knowledge of European fu- sion researchers regarding the Joint European Torus (JET) but that was a classic understatement. The meeting was a fully-fledged overview on JET’s capabilities which have tremendously changed in the past. The tokamak has gone through major upgrades since it saw its first deuterium tritium campaign in 1997. Those include not only an ITER-like wall but also an Fusion Writers… wanted! … increase of the heating power by 50 percent. -
Introduction to Nuclear Fusion
Introduction to Nuclear Fusion Prof. Dr. Yong-Su Na To build a sun on earth - Open magnetic confinement - Closed magnetic confinement 2 What is closed magnetic confinement? 3 Open Magnetic System B sin 2 min Bmax v|| loss cone loss cone - Suffering from end losses J.P. Freidberg, “Ideal Magneto-Hydro-Dynamics”, lecture note A. A. Harms et al, “Principles of Fusion Energy”, World Scientific (2000) 4 Open Magnetic System Magnetic field Is this motion realistic? ion Dunkin donuts (2010) 5 Closed Magnetic System Magnetic field Donut-shaped vacuum vessel ion 6 Closed Magnetic System 7 Closed Magnetic System Magnetic field R 0 a Plasma needs to be confined ion R0 = 1.8 m, a = 0.5 m in KSTAR 8 Closed Magnetic System Magnetic field R 0 a Plasma needs to be confined ion R0 = 6.2 m, a = 2.0 m in ITER 9 Closed Magnetic System Toroidal Field (TF) coil Magnetic field Toroidal direction Applying toroidal magnetic field ion 3.5 T in KSTAR, 5.3 T in ITER 10 Closed Magnetic System Toroidal Field (TF) coil Toroidal direction Applying toroidal magnetic field 3.5 T in KSTAR, 5.3 T in ITER 11 Closed Magnetic System Toroidal Field (TF) coil Magnetic field Toroidal direction Magnetic field of earth? 0.5 Gauss = 0.00005 T ion 12 http://www.crystalinks.com/earthsmagneticfield.html Closed Magnetic System Magnetic field Magnetic field of earth? 0.5 Gauss = 0.00005 T ion http://www.transformacionconciencia.com/archives/2384 13 Closed Magnetic System Magnetic field ion 14 Lesch, Astrophysics, IPP Summer School (2008) Closed Magnetic System Magnetic field ion electron -
Neutron Emission Spectrometry for Fusion Reactor Diagnosis
Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 1244 Neutron Emission Spectrometry for Fusion Reactor Diagnosis Method Development and Data Analysis JACOB ERIKSSON ACTA UNIVERSITATIS UPSALIENSIS ISSN 1651-6214 ISBN 978-91-554-9217-5 UPPSALA urn:nbn:se:uu:diva-247994 2015 Dissertation presented at Uppsala University to be publicly examined in Polhemsalen, Ångströmlaboratoriet, Lägerhyddsvägen 1, Uppsala, Friday, 22 May 2015 at 09:15 for the degree of Doctor of Philosophy. The examination will be conducted in English. Faculty examiner: Dr Andreas Dinklage (Max-Planck-Institut für Plasmaphysik, Greifswald, Germany). Abstract Eriksson, J. 2015. Neutron Emission Spectrometry for Fusion Reactor Diagnosis. Method Development and Data Analysis. Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 1244. 92 pp. Uppsala: Acta Universitatis Upsaliensis. ISBN 978-91-554-9217-5. It is possible to obtain information about various properties of the fuel ions deuterium (D) and tritium (T) in a fusion plasma by measuring the neutron emission from the plasma. Neutrons are produced in fusion reactions between the fuel ions, which means that the intensity and energy spectrum of the emitted neutrons are related to the densities and velocity distributions of these ions. This thesis describes different methods for analyzing data from fusion neutron measurements. The main focus is on neutron spectrometry measurements, using data used collected at the tokamak fusion reactor JET in England. Several neutron spectrometers are installed at JET, including the time-of-flight spectrometer TOFOR and the magnetic proton recoil (MPRu) spectrometer. Part of the work is concerned with the calculation of neutron spectra from given fuel ion distributions. -
Plasma Physics Laboratory
fco^m OCTOBER 1980 UC-20b,d NON-SUPERCONDUCTING- MAGNET STRUCTURES FOR NEAR^TEfti LARGE FUSION EXPERIMENTAL DEVICES -:BY J. FILE, D. S, KHUT^xiU, R, E, MARINO, AND G. ti, RAPPE PLASMA PHYSICS LABORATORY r,7 PRINCETON UNIVERSITY PRINCETON, NEW JERSEY m tr T;;;S 30CUV£MT !S iHnwrru NON-SUPERCONDUCTING MAGNET STRUCTURES FOR NBRR-'IERM, LARGE FUSION EXPERIMENTAL DEVICES J. File, D.S. Knutson, R.E. Marino and G.H. Rappe Plasma Physics Laboratory, Princeton University, Princeton, New Jersey 08544, USA ABSTRACT Water cooled copper magnets provide a means of producing high magnetic fields for tokamaks using a well developed existing technology. The basic function of these magnets is to provide reliable, both time varying and steady state, magnetic fields. Copper electrical properties, insulation, and water cooling systems play major roles in design selection. Aside from being electro-magnetic devices, coils designed for tokamaks must be self-supporting structures, capable of resisting large I x B magnetic forces. These magnets require the integration of both electrical and structural design considerations. Magnet integrity is enhanced by the presence of structures which lend additional external support. These external structural systems are highly stressed and, often, deflection limited. This paper describes the magnet and structural design in the following American tokamak devices: the Princeton Large Torus (PLT), the Princeton Divertor Experiment (PDX), and the Tokamak Fusion Test Reactor (TFTR). The Joint European Torus (JET), also presented herein, has a magnet structure evolved from several European programs and, like TFTR, represents state of the art magnet and structure design. | DISCLAIMER TliTtbOGknA!}!K>£!K!ajn*^oun1i''M?l looniofeo cyan Jgency of fifl Unrie-J Slaftt Gowmrien*. -
Fusion Energy Source of the Future
Fusion Energy Source of the Future EUROfusion Research Progamme in Austria 2014 - 2020 Impressum Editors Monika Fischer [email protected] Lätitia Unger [email protected] Friedrich Aumayr [email protected] Contributions from Friedrich Aumayr, Markus Biberacher, Lukas Einkemmer, Michael Eisterer, Codrina Ionita-Schrittwieser, Alexander Kendl, Winfried Kernbichler, Helmut Leeb, Reinhard Pippan, Michael Probst, Paul Scheier, Klaus Schöpf, Roman Schrittwieser, David Tskhakaya Acknowledgements Austrian Academy of Sciences: Bernhard Plunger, Anton Zeilinger and Presiding Committee Federal Ministry of Education, Science and Research: Stefan Hanslik, Daniel Weselka Kommission für die Koordination der Kernfusionsforschung in Österreich (KKKÖ): Peter Steinhauser (chair), Friedrich Aumayr, Michael Eisterer, Alexander Kendl, Helmut Leeb, Winfried Kernbichler, Harald Weber, Daniel Weselka Financial Support Federal Ministry of Education, Science and Research, Austrian Academy of Sciences EUROfusion Co-Fund Action (H2020 Grant No. 633053) Disclaimer EUROfusion receives funding from Euratom’s research and training programme 2014-2018 and 2019-2020 under Grant Agreement No. 633053 and finances fusion research activities in accordance with the Roadmap to the realisation of fusion energy. The views and opinions expressed herein do not necessarily reflect those of the European Commission. Cover image: ITER Tokamak and Plant Systems (Credit: www.ITER.org) Fusion Energy Source of the Future EUROfusion Research Programme in Austria, 2014-2020 Editors: Monika Fischer, Lätitia Unger Friedrich Aumayr Supported by: Copyright © 2020 by Austrian Academy of Sciences Vienna Printed in Austria Table of Contents Page EXECUTIVE SUMMARY 2 ZUSAMMENFASSUNG 4 1. Management Structure and Core Competencies 7 1.1. EUROfusion Consortium 7 1.2. Austrian Beneficiary ÖAW and its Linked Third Parties 7 2. -
Sixty Years on from ZETA …
Sixty years on from ZETA … Chris Warrick The Sun … What is powering it? Coal? Lifetime 3,000 years Gravitational Energy? Lifetime 30 million years – Herman Von Helmholtz, Lord Kelvin - mid 1800s The Sun … Suggested the Earth is at least 300 million years old – confirmed by geologists studying rock formations … The Sun … Albert Einstein (Theory of Special Relativity) and Becquerel / Curie’s work on radioactivity – suggested radioactive decay may be the answer … But the Sun comprises hydrogen … The Sun … Arthur Eddington proposed that fusion of hydrogen to make helium must be powering the Sun “If, indeed, the subatomic energy is being freely used to maintain their great furnaces, it seems to bring a little nearer to fulfilment our dream of controlling this latent power for the well-being of the human race – or for its suicide” Cambridge – 1930s Cockcroft Walton accelerator, Cavendish Laboratory, Cambridge. But huge energy losses and low collisionality Ernest Rutherford : “The energy produced by the breaking down of the atom is a very poor kind of thing . Anyone who expects a source of power from the transformation of these atoms is talking moonshine.” Oxford – 1940s Peter Thonemann – Clarendon Laboratory, Oxford. ‘Pinch’ experiment in glass, then copper tori. First real experiments in sustaining plasma and magnetically controlling them. Imperial College – 1940s George Thomson / Alan Ware – Imperial College London then Aldermaston. Also pinch experiments, but instabilities started to be observed – especially the rapidly growing kink instability. AERE Harwell Atomic Energy Research Establishment (AERE) Harwell – Hangar 7 picked up fusion research. Fusion is now classified. Kurchatov visit 1956 ZETA ZETA Zero Energy Thermonuclear Apparatus Pinch experiment – but with added toroidal field to help with instabilities and pulsed DC power supplies. -
Plasma Physics and Controlled Fusion Research During Half a Century Bo Lehnert
SE0100262 TRITA-A Report ISSN 1102-2051 VETENSKAP OCH ISRN KTH/ALF/--01/4--SE IONST KTH Plasma Physics and Controlled Fusion Research During Half a Century Bo Lehnert Research and Training programme on CONTROLLED THERMONUCLEAR FUSION AND PLASMA PHYSICS (Association EURATOM/NFR) FUSION PLASMA PHYSICS ALFV N LABORATORY ROYAL INSTITUTE OF TECHNOLOGY SE-100 44 STOCKHOLM SWEDEN PLEASE BE AWARE THAT ALL OF THE MISSING PAGES IN THIS DOCUMENT WERE ORIGINALLY BLANK TRITA-ALF-2001-04 ISRN KTH/ALF/--01/4--SE Plasma Physics and Controlled Fusion Research During Half a Century Bo Lehnert VETENSKAP OCH KONST Stockholm, June 2001 The Alfven Laboratory Division of Fusion Plasma Physics Royal Institute of Technology SE-100 44 Stockholm, Sweden (Association EURATOM/NFR) Printed by Alfven Laboratory Fusion Plasma Physics Division Royal Institute of Technology SE-100 44 Stockholm PLASMA PHYSICS AND CONTROLLED FUSION RESEARCH DURING HALF A CENTURY Bo Lehnert Alfven Laboratory, Royal Institute of Technology S-100 44 Stockholm, Sweden ABSTRACT A review is given on the historical development of research on plasma physics and controlled fusion. The potentialities are outlined for fusion of light atomic nuclei, with respect to the available energy resources and the environmental properties. Various approaches in the research on controlled fusion are further described, as well as the present state of investigation and future perspectives, being based on the use of a hot plasma in a fusion reactor. Special reference is given to the part of this work which has been conducted in Sweden, merely to identify its place within the general historical development. Considerable progress has been made in fusion research during the last decades.