Inertial Confinement Fusion
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
The Next Generation of Fusion Energy Research
THE NEXT GENERATION OF FUSION ENERGY RESEARCH HEARING BEFORE THE SUBCOMMITTEE ON ENERGY AND ENVIRONMENT COMMITTEE ON SCIENCE AND TECHNOLOGY HOUSE OF REPRESENTATIVES ONE HUNDRED ELEVENTH CONGRESS FIRST SESSION OCTOBER 29, 2009 Serial No. 111–61 Printed for the use of the Committee on Science and Technology ( Available via the World Wide Web: http://www.science.house.gov U.S. GOVERNMENT PRINTING OFFICE 52–894PDF WASHINGTON : 2010 For sale by the Superintendent of Documents, U.S. Government Printing Office Internet: bookstore.gpo.gov Phone: toll free (866) 512–1800; DC area (202) 512–1800 Fax: (202) 512–2104 Mail: Stop IDCC, Washington, DC 20402–0001 COMMITTEE ON SCIENCE AND TECHNOLOGY HON. BART GORDON, Tennessee, Chair JERRY F. COSTELLO, Illinois RALPH M. HALL, Texas EDDIE BERNICE JOHNSON, Texas F. JAMES SENSENBRENNER JR., LYNN C. WOOLSEY, California Wisconsin DAVID WU, Oregon LAMAR S. SMITH, Texas BRIAN BAIRD, Washington DANA ROHRABACHER, California BRAD MILLER, North Carolina ROSCOE G. BARTLETT, Maryland DANIEL LIPINSKI, Illinois VERNON J. EHLERS, Michigan GABRIELLE GIFFORDS, Arizona FRANK D. LUCAS, Oklahoma DONNA F. EDWARDS, Maryland JUDY BIGGERT, Illinois MARCIA L. FUDGE, Ohio W. TODD AKIN, Missouri BEN R. LUJA´ N, New Mexico RANDY NEUGEBAUER, Texas PAUL D. TONKO, New York BOB INGLIS, South Carolina PARKER GRIFFITH, Alabama MICHAEL T. MCCAUL, Texas STEVEN R. ROTHMAN, New Jersey MARIO DIAZ-BALART, Florida JIM MATHESON, Utah BRIAN P. BILBRAY, California LINCOLN DAVIS, Tennessee ADRIAN SMITH, Nebraska BEN CHANDLER, Kentucky PAUL C. BROUN, Georgia RUSS CARNAHAN, Missouri PETE OLSON, Texas BARON P. HILL, Indiana HARRY E. MITCHELL, Arizona CHARLES A. WILSON, Ohio KATHLEEN DAHLKEMPER, Pennsylvania ALAN GRAYSON, Florida SUZANNE M. -
7 Upgrade to the Vulcan Laser System to Support the TAW Upgrade
LASER SCIENCE AND DEVELOPMENT I Vulcan 7 Upgrade to the Vulcan laser system to support the TAW upgrade Contact [email protected] B. T. Parry, T. B. Winstone, P. N. Anderson, A. J. Frackiewicz, M. Galimberti, S. Hancock, C. Hernandez-Gomez, A. K. Kidd, M. M. Notley, M. Read and C. Wise Central Laser Facility, STFC, Rutherford Appleton Laboratory, HSIC, Didcot, Oxon OX11 0QX, UK Introduction chains. One of the rod amplifier beam lines is split The Vulcan laser facility has recently been upgraded to into two to form beams 7 and 8, the other is split into deliver an additional short pulse beam to Target Area beams 1-6. Beams 7 and 8 are normally used as short West (TAW) [1]. This new beamline is capable of pulse (CPA) beamlines. operating in the same mode as the previously existing Modelling showed that the extra amplification needed one, at energies up to 100 J in 1 ps. It also allows the to deliver the increased energy could be carried out at laser to reach new, previously inaccessible regimes, smaller beam diameter while still keeping the B-integral with the capability to deliver up to 500 J in pulses of below three, the limit for what was acceptable for a 10 ps or longer (100ps max). 10 ps pulse. This meant that rod amplifiers, rather than The increase in the delivered energy was made possible large, costly disk amplifiers, could be used. An by the use of dielectric gratings for this new 10 ps additional 45 mm diameter rod amplifier was installed beamline. -
Fusion Energy Science Opportunities in Emerging Concepts
Fusion Energy Science Opportunities in Emerging Concepts Los Alamos National Laboratory Report -- LA-UR-99-5052 D. C. Barnes Los Alamos National Laboratory For the Emerging Concepts Working Group Convenors: J. Hammer Lawrence Livermore National Laboratory A. Hassam University of Maryland D. Hill Lawrence Livermore National Laboratory A. Hoffman University of Washington B. Hooper Lawrence Livermore National Laboratory J. Kesner Massachusetts Institute of Technology G. Miley University of Illinois J. Perkins Lawrence Livermore National Laboratory D. Ryutov Lawrence Livermore National Laboratory J. Sarff University of Wisconsin R. E. Siemon Los Alamos National Laboratory J. Slough University of Washington M. Yamada Princeton Plasma Physics Laboratory I. Introduction The development of fusion energy represents one of the few long-term (multi-century time scale) options for providing the energy needs of modern (or postmodern) society. Progress to date, in parameters measuring the quality of confinement, for example, has been nothing short of stellar. While significant uncertainties in both physics and (particularly) technology remain, it is widely believed that a fusion reactor based on the tokamak could be developed within one or two decades. It is also widely held that such a reactor could not compete economically in the projected energy market. A more accurate statement of projected economic viability is that the uncertainty in achieving commercial success is sufficient that the large development costs required for such a program are not justified at this time. While technical progress has been spectacular, schedule estimates for achieving particular milestones along the path of fusion research and development have proven notoriously inaccurate. This inaccuracy reflects two facts. -
1958 Geneva Conference on the Discontinuation of Nuclear Weapons
1 2 3 4 5 6 7 8 Presidential Decisions on Stockpile Stewardship Test-Based Stewardship and the Cold War Transitioning to Stockpile Stewardship Science: Research, Development, and Technology Deterrence and the Life Extension Program Global Nuclear Security Timeline of U.S. Stockpile Stewardship Innovation The Path Forward Today, I am announcing my “decision to negotiate a true zero-yield comprehensive test ban.” U.S. President Bill Clinton, August 11, 1995 The National Defense Authorization Act for fiscal year 1994 (P.L. 103-160) estab- lished the Stockpile Stewardship Program (SSP) to sustain the nuclear deterrent in the absence of nuclear explosive testing. The SSP supports U.S. national security missions through leading-edge scientific, engineering, and technical tools and expertise – a U.S. response to the end of the Cold War and the need to remake the global nuclear landscape. One year later, on August 11, 1995, Presi- dent Bill Clinton announced that the United States would support a “zero yield” Compre- hensive Nuclear-Test-Ban Treaty (CTBT): “I am assured by the Secretary of Energy and the Directors of our nu- clear weapons labs that we can meet the challenge of maintaining our nuclear deterrent under a Compre- hensive Test-Ban Treaty through a Science-Based Stockpile Stewardship program without nuclear testing.” This year, the Nation and the Department of Energy (DOE) celebrate the 20th anniver- sary of that announcement and the scientific and technical capabilities that have devel- oped to support this policy direction. The national investment in stockpile stewardship has enabled resolution of many stockpile issues and provided more detailed knowledge than what could have been attained through nuclear explosive testing. -
A Fusion Test Facility for Inertial Fusion
A Fusion Test Facility for Inertial Fusion The Fusion Test Facility would be part of an integrated IFE program where the essential elements are developed and implemented as systems in progressively more capable IFE oriented facilities. Fusion Test Facility (FTF) Direct laser drive Sub-megaJoule laser energy Goal of ~150 MW fusion power High flux neutron source Development path to a power plant Presented by Stephen Obenschain U.S. Naval Research Laboratory September 27 2006 Fusion Power Associates Meeting Introduction The scientific underpinnings for ICF has and is being developed via large single shot facilities. The IFE application, while greatly benefiting from this effort, requires a different and broader perspective. • Development of sufficiently efficient and durable high repetition rate drivers. • High gain target designs consistent with the energy application. • Development of economical mass production techniques for targets. • Precision target injection, tracking & laser beam steering. • Reaction chamber design and materials for a harsh environment. • Operating procedures (synchronizing a complex high duty cycle operation) • Overall economics, development time and costs. Individual IFE elements have conflicts in their optimization, and have to be developed in concert with their own purpose-built facilities. HAPL= $25M/yr High Average Power Laser program administered by NNSA See presentations by John Sethian and John Caird this afternoon. Typical GW (electrical )designs have >3 MJ laser drivers @ 5-10 Hz Target Factory Electricity -
Part 1: April 24, 2007 Presentations
UCRL-MI-231268 IFE Science and Technology Strategic Planning Workshop - Part 1: April 24, 2007 Presentations To select an individual presentation, click the table of contents entry on the next page or click the title on the agenda for Day 1 (using the Hand Tool icon). To save only a portion of this document, go to File/Print, select Adobe PDF as your printer, specify the desired range of pages, and save to a new file name. This document was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor the University of California nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or the University of California. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or the University of California, and shall not be used for advertising or product endorsement purposes. Portions of this work performed under the auspices of the U. S. Department of Energy by University of California Lawrence Livermore National Laboratory under Contract W-7405-Eng-48. Part 1 Contents Agenda ........................................................................................................................................ 3 Presentations 1. Welcome and Perspectives, Ed Synakowski, LLNL............................................................ -
Een Kernfusie Concept
Kernfusie Dr. Robert Bussard over kernfusie http://video.google.com/videoplay?docid=1996321846673788606# In de bovenstaande link geeft Robert Bussard een conferentie over alternatieve fusie energie waar hij zijn alternatieve opstelling “de polywell” verdedigt. Hoewel de benadering tot kernfusie in dit document geheel anders is, is het doel en sommige basisprincipes hetzelfde en had ik het zelf niet beter kunnen verwoorden. De opstelling De opstelling bestaat uit een sferische tank die doormiddel van een mechanisch systeem (fig1) wordt rondgedraaid, dit in twee dimensies. Het rondspinnen om twee assen van het lichaam zorgt ervoor dat deeltjes met de hoogste massadichtheid naar buiten worden geslingerd. De deeltjes met de laagste dichtheid worden hierdoor naar het center gedrukt. Als er dus bijvoorbeeld water in de sfeer bevindt, zal deze homogeen over de binnenkant van de sferische wand worden gedrukt. De lichtere, eventueel hetere deeltjes worden in het center gehouden. Warmteconvectie wordt hierdoor onderdrukt. Dit maakt dat het plasma geïsoleerd is zonder dat er een vacuüm kamer noodzakelijk is. Zoals bij een Tokamak, Stellator, Fusor of polywell wel het geval is. Hierdoor kan de druk in het plasma makkelijk opgevoerd worden zonder dat er super magneten voor noodzakelijk zijn, simpel weg door statische druk. Dit zou een drastisch verschil moeten maken in energiedichtheid. De opgewekte energie stijgt kwadratisch met De figuur 1: Het draaimechanisme de druk. Tevens kunnen er energieke geladen plasma deeltjes geïnjecteerd worden, wat bij magnetische opsluiting niet mogelijk is. sferische tank met daar rond het draaimechanisme bevindt zich in een tweede robuustere tank die bestand is tegen hoge druk. De vrijgekomen energie wordt afgevoerd voordat het de reactorwand bereikt evenals de 14Mev neutronen worden gemodereerd. -
NRL Nike Laser Focuses on Nuclear Fusion 20 March 2013
NRL Nike Laser focuses on nuclear fusion 20 March 2013 concept, numerous laser beams are used to implode and compress a pea-sized pellet of deuterium-tritium (D-T) to extreme density and temperature, causing the atoms to fuse, resulting in the release of excess energy. In an ICF implosion, a progressively diminishing portion of the beams will engage the shrinking pellet if the focal spot diameter of the laser remains unchanged. For optimal coupling, it becomes desirable to decrease the laser focal spot size to match the reduction in the pellet's diameter, minimizing wasted energy. This is the Nike Laser -- focal zooming. Credit: U.S. "Matching the focal spot size to the pellet Naval Research Laboratory throughout the implosion process maximizes the on- target laser energy," Kehne said. "This experiment validates the engineering of focal zooming in KrF lasers to track the size of an imploding pellet in Researchers at the U.S. Naval Research inertial confinement fusion." Laboratory have successfully demonstrated pulse tailoring, producing a time varying focal spot size With single-step focal zooming implemented, the known as 'focal zooming' on the world's largest Nike laser provides independent control of pulse operating krypton fluoride (KrF) gas laser. shape, time of arrival, and focal diameter allowing greater flexibility in the profiles and pulse shapes The Nike laser is a two to three kilojoule (kJ) KrF that can be produced. The flexibility in pulse system that incorporates beam smoothing by shaping provides promising uses in both future induced spatial incoherence (ISI) to achieve one experiments and laser diagnosis. -
Minimization of Magnetic Forces on Stellarator Coils Arxiv:2103.13195
Minimization of magnetic forces on Stellarator coils R´emiRobin∗; 1 and Francesco Volpe †2 1 Laboratoire Jacques-Louis Lions, Sorbonne Universit´e 2Renaissance Fusion, https://stellarator.energy March 25, 2021 Abstract Magnetic confinement devices for nuclear fusion can be large and expensive. Compact stellarators are promising candidates for cost- reduction, but introduce new difficulties: confinement in smaller vol- umes requires higher magnetic field, which calls for higher coil-currents and ultimately causes higher Laplace forces on the coils - if everything else remains the same. This motivates the inclusion of force reduction in stellarator coil optimization. In the present paper we consider a coil winding surface, we prove that there is a natural and rigorous way to define the Laplace force (despite the magnetic field discontinuity across the current-sheet), we provide examples of cost associated (peak force, surface-integral of the force squared) and discuss easy generalizations to parallel and normal force-components, as these will be subject to different engineering constraints. Such costs can then be easily added arXiv:2103.13195v1 [math.OC] 24 Mar 2021 to the figure of merit in any multi-objective stellarator coil optimiza- tion code. We demonstrate this for a generalization of the REGCOIL code [1], which we rewrote in python, and provide numerical examples for the NCSX (now QUASAR) design. We present results for various definitions of the cost function, including peak force reductions by up to 40 %, and outline future work for further reduction. ∗[email protected] †[email protected] 1 1 Introduction Stellarators are non-axisymmetric toroidal devices that magnetically confine fusion plasmas [2]. -
Nd Lu Caf2 for High-Energy Lasers Simone Normani
Nd Lu CaF2 for high-energy lasers Simone Normani To cite this version: Simone Normani. Nd Lu CaF2 for high-energy lasers. Physics [physics]. Normandie Université, 2017. English. NNT : 2017NORMC230. tel-01689866 HAL Id: tel-01689866 https://tel.archives-ouvertes.fr/tel-01689866 Submitted on 22 Jan 2018 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. THESE Pour obtenir le diplôme de doctorat Physique Préparée au sein de l’Université de Caen Normandie Nd:Lu:CaF2 for High-Energy Lasers Étude de Cristaux de CaF2:Nd:Lu pour Lasers de Haute Énergie Présentée et soutenue par Simone NORMANI Thèse soutenue publiquement le 19 octobre 2017 devant le jury composé de M. Patrice CAMY Professeur, Université de Caen Normandie Directeur de thèse M. Alain BRAUD MCF HDR, Université de Caen Normandie Codirecteur de thèse M. Jean-Luc ADAM Directeur de Recherche, CNRS Rapporteur Mme. Patricia SEGONDS Professeur, Université de Grenoble Rapporteur M. Jean-Paul GOOSSENS Ingénieur, CEA Examinateur M. Maurizio FERRARI Directeur de Recherche, CNR-IFN Examinateur Thèse dirigée par Patrice CAMY et Alain BRAUD, laboratoire CIMAP Université de Caen Normandie Nd:Lu:CaF2 for High-Energy Lasers Thesis for the Ph.D. -
Memorandum to Participants JASON 1994 Summer Study
Hydronnclear Testing and the Comprehensive Test Ban: Memorandum to Participants JASON 1994 Summer Study Natural Resources Defense Council, Inc. 1350 New York Avenue, NW, Suite 300 Washington, D.C. 20005 Tel (main): (202) 783-7800 Cochran (direct dial): (202) 624-9329 Paine (direct dial): (202) 624-9350 Fax: (202) 783-5917 INTERNET: [email protected] Although no commonly accepted defInition exists, a "hydronuclear test" may be generally described as a nuclear weapons test, or high-explosive driven criticality experiment, characterized by a nuclear energy release that is insuffIcient to heat the core material to the plasma temperatures that would cause it to explode "like a bomb." In such a test, the TNT equivalent energy release from fission would therefore not exceed the amount released by the chemical high explosive used to compress the fIssile material, and could be considerably ,less. Nuclear-weapon states, and possibly other states, also perform high-explosive driven implosion experiments using fusjon material, although" these' are not nonnally characterized as "hydronuclear tests". Hydronuclear tests can serve a useful role in the development of the full spectrum of unboosted fIssion weapons, including'first generation nuclear weapons of the implosion type with yields in the 5 to 30 kiloton range, more sophisticated designs with yields up to about a megaton, and advanced micro-nuclear weapons with yields of 5 to 500 tons. For pure fIssion weapons hydronuclear tests can be used to:' * optimize the timing of initiation of the -
Advanced Approaches to High Intensity Laser-Driven Ion Acceleration
Advanced Approaches to High Intensity Laser-Driven Ion Acceleration Andreas Henig M¨unchen2010 Advanced Approaches to High Intensity Laser-Driven Ion Acceleration Andreas Henig Dissertation an der Fakult¨atf¨urPhysik der Ludwig{Maximilians{Universit¨at M¨unchen vorgelegt von Andreas Henig aus W¨urzburg M¨unchen, den 18. M¨arz2010 Erstgutachter: Prof. Dr. Dietrich Habs Zweitgutachter: Prof. Dr. Toshiki Tajima Tag der m¨undlichen Pr¨ufung:26. April 2010 Contents Contentsv List of Figures ix Abstract xiii Zusammenfassung xv 1 Introduction1 1.1 History and Previous Achievements...................1 1.2 Envisioned Applications.........................3 1.3 Thesis Outline...............................5 2 Theoretical Background9 2.1 Ionization.................................9 2.2 Relativistic Single Electron Dynamics.................. 14 2.2.1 Electron Trajectory in a Linearly Polarized Plane Wave.... 15 2.2.2 Electron Trajectory in a Circularly Polarized Plane Wave... 17 2.2.3 Electron Ejection from a Focussed Laser Beam......... 18 2.3 Laser Propagation in a Plasma..................... 18 2.4 Laser Absorption in Overdense Plasmas................. 20 2.4.1 Collisional Absorption...................... 20 2.4.2 Collisionless Absorption..................... 21 2.5 Ion Acceleration.............................. 22 2.5.1 Target Normal Sheath Acceleration (TNSA).......... 22 2.5.2 Shock Acceleration........................ 26 2.5.3 Radiation Pressure Acceleration / Light Sail / Laser Piston. 27 3 Experimental Methods I - High Intensity Laser Systems 33 3.1 Fundamentals of Ultrashort High Intensity Pulse Generation..... 33 vi CONTENTS 3.1.1 The Concept of Mode-Locking.................. 33 3.1.2 Time-Bandwidth Product.................... 37 3.1.3 Chirped Pulse Amplification................... 39 3.1.4 Optical Parametric Amplification (OPA)............ 40 3.2 Laser Systems Utilized for Ion Acceleration Studies.........