Historical Perspective on the United States Fusion Program
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Nova Laser Technology
Nova Laser Technology In building the Nova laser, we have significantly advanced many technologies, including the generation and propagation of laser beams. We have also developed innovations in the fields of alignment, diagnostics, computer control, and image processIng.• For further information contact Nova is the world's most powerful at least 10 to 30 times more energetic John F. Holzrichter (415) 423-7454. laser system. It is designed to heat and than Shiva would be needed to compress small targets, typically 0.1 cm investigate ignition conditions and in size, to conditions otherwise produced possibly to reach gains near unity. only in nuclear weapons or in the Because of the importance of such a interior of stars. Its beams can facility to the progress of inertial fusion concentrate 80 to 120 kJ of energy (in research and because of the construction 3 ns) or 80 to 120 TW of power (in time entailed (at least five to seven 100 ps) on such targets. To couple energy years), the Nova project was proposed to more favorably with the target, Nova's the Energy Research and Development laser light will be harmonically converted Administration and to Congress. It was with greater than 50% efficiency from its decided to base this system on the near-infrared fundamental wavelength proven master-oscillator, linear-amplifier (1.05-,um wavelength) to green (0.525- chain laser system used on the Argus ,um) or blue (0.35-,um) wavelengths. The and Shiva systems. We had great goals of our experiments with Nova are confidence in extending this to make accurate measurements of high neodymium-glass laser technology to the temperature and high-pressure states of 200- to 300-kJ level. -
ENGINEERING DESIGN of the NOVA LASER FACILITY for By
ENGINEERING DESIGN OF THE NOVA LASER FACILITY FOR INERTIAL-CONFINEMENT FUSION* by W. W. Simmons, R. 0. Godwin, C. A. Hurley, E. P. Wallerstein, K. Whitham, J. E. Murray, E. S. Bliss, R. G. Ozarski. M. A. Summers, F. Rienecker, D. G. Gritton, F. W. Holloway, G. J. Suski, J. R. Severyn, and the Nova Engineering Team. Abstract The design of the Nova Laser Facility for inertia! confinement fusion experiments at Lawrence Livermore National Laboratory is presented from an engineering perspective. Emphasis is placed upon design-to- performance requirements as they impact the various subsystems that comprise this complex experimental facility. - DISCLAIMER - CO;.T-CI104n--17D DEf;2 013.375 *Research performed under the auspices of the U.S. Department of Energy by the Lawrence Livermore National Laboratory under contract number W-7405-ENG-48. Foreword The Nova Laser System for Inertial Confinement Fusion studies at Lawrence Livermore National Laboratories represents a sophisticated engineering challenge to the national scientific and industrial community, embodying many disciplines - optical, mechanical, power and controls engineering for examples - employing state-of-the-art components and techniques. The papers collected here form a systematic, comprehensive presentation of the system engineering involved in the design, construction and operation of the Nova Facility, presently under construction at LLNL and scheduled for first operations in 1985. The 1st and 2nd Chapters present laser design and performance, as well as an introductory overview of the entire system; Chapters 3, 4 and 5 describe the major engineering subsystems; Chapters 6, 7, 8 and 9 document laser and target systems technology, including optical harmonic frequency conversion, its ramifications, and its impact upon other subsystems; and Chapters 10, 11, and 12 present an extensive discussion of our integrated approach to command, control and communications for the entire system. -
Lasers Join the Quest for Fusion Energy
1974 Lasers and ICF Lasers Join the Quest to gain a better understanding of laser plasma physics and thermonuclear physics and to demonstrate for Fusion Energy laser-induced compression and thermonuclear burn of deuterium–tritium. It was also used to improve the LASNEX computer code developed for laser With the goal of achieving energy gain fusion predictions. Janus was just the In 1975, the one-beam Cyclops laser through inertial confinement fusion beginning of the development, in quick began operation, performing important (ICF) as its mission, the Laser Program succession, of a series of lasers, each target experiments and testing optical constructed its first laser for ICF building on the knowledge gained from designs for future lasers. The next year, experiments in 1974. Named Janus, the last, leading to the National Ignition the two-beam Argus was built. Use of the two-beam laser was built with about Facility (NIF), currently performing Argus increased knowledge about laser– 100 pounds of laser glass. experiments. The pace of laser target interactions and laser propagation The first Livermore laser for construction matched the growth limits, and it helped the ICF program prepared the Laboratory to take the With the 20-beam ICF research, Janus, had Under the leadership of John Emmett, in ICF diagnostics capabilities, develop technologies needed for the next major step, construction of the Shiva laser in 1977, the two beams and produced who headed the Laser Program from computer simulation tools, and next generation of laser fusion systems. 192-beam NIF (see Year 1997), where Laboratory established 10 joules of energy. -
The Effect of Surface Processing Methods on the Laser Induced Damage Threshold of Fused Silica
The Effect of Surface Processing Methods on the Laser Induced Damage Threshold of Fused Silica by Weiran Duan A thesis submitted in partial fulfilment for the requirements for the degree of PhD at the University of Central Lancashire October 2014 2 To my family i Declaration I declare that while registered as a candidate for the research degree, I have not been a registered candidate or enrolled student for another award of the University or other academic or professional institution. I declare that no material contained in the thesis has been used in any other submission for an academic award and is solely my own work. Weiran Duan ii Abstract High peak power laser systems, such as National Ignition Facility (NIF), Laser Mega Joule (LMJ), and High Power laser Energy Research facility (HiPER), include a large amount of optics. Fused silica glass is one of the most common optical materials which is used in these high peak power laser systems owing to its excellent optical properties, especially for the 355nm ultraviolet laser. However, it is generally found that fused silica optics damage under irradiation with a high peak power laser beam, and the laser induced damage (LID) becomes the limit to increasing the laser power. Theoretically, the laser induced damage threshold (LIDT) of fused silica substrates is high, while it drops significantly due to the poor surface quality created in the manufacturing process. This project aims to find a series of fused silica optical surface processing techniques which are able to improve the surface quality and increase its LIDT when irradiated using high peak power lasers. -
Nuclear Diagnostics for Inertial Confinement Fusion (ICF) Plasmas
PSFC/JA-20-4 Nuclear diagnostics for Inertial Confinement Fusion (ICF) plasmas J. A. Frenje January 2020 Plasma Science and Fusion Center Massachusetts Institute of Technology Cambridge MA 02139 USA The work described herein was supported in part by US DOE (Grant No. DE-FG03-03SF22691), LLE (subcontract Grant No. 412160-001G) and the Center for Advanced Nuclear Diagnostics (Grant No. DE-NA0003868). Reproduction, translation, publication, use and disposal, in whole or in part, by or for the United States government is permitted. Submitted to Plasma Physics and Controlled Fusion Nuclear Diagnostics for Inertial Confinement Fusion (ICF) Plasmas J.A. Frenje1 1Massachusetts Institute of Technology, Cambridge, MA 02139, USA Email: [email protected] The field of nuclear diagnostics for Inertial Confinement Fusion (ICF) is broadly reviewed from its beginning in the seventies to present day. During this time, the sophistication of the ICF facilities and the suite of nuclear diagnostics have substantially evolved, generally a consequence of the efforts and experience gained on previous facilities. As the fusion yields have increased several orders of magnitude during these years, the quality of the nuclear-fusion-product measurements has improved significantly, facilitating an increased level of understanding about the physics governing the nuclear phase of an ICF implosion. The field of ICF has now entered an era where the fusion yields are high enough for nuclear measurements to provide spatial, temporal and spectral information, which have proven indispensable to understanding the performance of an ICF implosion. At the same time, the requirements on the nuclear diagnostics have also become more stringent. -
Lll Laser Program Overview
I ~ Ellerll APR 13 1~76 ~ illid ~~WJF Destroy Telllllllllill Route - Hold mos. Prepared for U.S . Energy Research & Development lell Administration under Contract No. W-7405-Eng-48 LA.WRENCE LIVERMORE LA.BORATORY LLL LASER PROGRAM LASERS AND LASER APPLICATIONS LLL LASER PROGRAM OVERVIEW ------------------------ During the past year, substantial progress has been thermonuclear burn of microscopic targets containing made toward laser fusion, laser isotope separation, and deuterium and tritium. Experiments are being run on the development of advanced laser media, the three a single-pulse basis , the emphasis being on fa st main thrusts of the LLL laser program. diagnostics of neutron, x-ray, a-particle, and scattered Our accomplishments in laser fusion have included: laser-light fluxes from the target. Our laser source fo r • Firing and diagnosing more than 650 individual this work is the neodymium-doped-glass (Nd:glass) experiments on the O.4-TW Janus laser system laser operating in a master-oscillator, power-amplifier (including many experiments with neutron yields in configuration, where a well-characterized, mode-locked the 107 range). pulse is shaped and ampli fied by successive stages to • Producing 1 TW of on-target irradiation with a peak power of I TW in a 20-cm-diam beam. Cyclops, presently the world's most powerful Thermonuclear burn has been demonstrated. With single-beam laser. successively larger Nd :glass laser systems, we now • Completing the design for the 25-TW Shiva laser expect sequentially to demonstrate significant burn, system and ordering the long-lead-time components. light energy breakeven (equal input and output (The building to house this laser system is on schedule energies) and, finally, net energy gain. -
Laser Confinement Fusion • Use Powerful Laser to Compress And
Laser Confinement Fusion • Use powerful laser to compress and heat hydrogen • Hydrogen stored in very small pellets • Outside of pellet boiled off by laser beam • Ablation causes plasma • Pellet compressed 4-5 times density of liquid hydrogen •Reaches temperature/pressure of sun core • Get Fusion reaction H 3 + H 2 → He4 + n +14MeV Laser Fusion Reactor • Pellets dropped into reactor • Laser pulse (40 nsec & terawatt) ignites compression wave • Energy from fusion carried in neutrons & helium 3 • Liquid Lithium shield adsorbs neutrons and energy • Regular "steam" generator to get power Argus Laser Fusion Facility • Lawrence Livermore Labs: 2 Terawatt in 1 nsec pulse • Nd:yag/glass laser built in 1976 • Demonstrated concepts for laser confinement fusion • Problem: need to have pellet heated very uniformly • Thus next stage increased number of beams Shiva Laser Fusion Facility • 20 Beam Nd:Yag system • Lawrence Livermore Labs: 30 Terawatt, 1 nsec • Most important result: needed to go to shorter wavelength National Ignition Facility • National Ignition Facility (NIF) newest design • 1.8 megaJoul, frequency tripled Nd:glass laser • 10 ps pulse, 1019 W/cm2 • 192 beam lines combined • Test concepts with Peta Wat laser • 1.25x1015W, 0.55 ps pulse, 1021 W/cm2 • Located at Lawrence Livermore Labs Laser Flight • Use orbital laser satellites to send down beams orbital solar power satellites • Light focused and tracts aircraft • Flight takes off normally - regular engines • Switches to laser drive for cruse section of flight • Significant savings in -
APPENDIX a Why Magnetized Target Fusion Offers a Low-Cost
MTF Proof-of-Principle Proposal App. A. Why MTF offers a low-cost development path. APPENDIX A Why Magnetized Target Fusion Offers A Low-Cost Development Path for Fusion Energy Richard E. Siemon Irvin R. Lindemuth Kurt F. Schoenberg Los Alamos National Laboratory Los Alamos, New Mexico Accepted by Comments on Plasma Physics and Controlled Fusion, December, 1997 1 MTF Proof-of-Principle Proposal App. A. Why MTF offers a low-cost development path. I. Introduction Reasonably priced energy supplies have become an expectation of the developed world and a necessary ingredient for development of Third World countries. The problem of providing large supplies of low-cost energy is a long-term, complex one that requires sustained R&D efforts, in spite of the shadow cast on long-term R&D by the federal deficit problem. The role of fusion energy as a power source was thoroughly reviewed and strongly endorsed in 1995 by the President’s Committee of Advisors on Science and Technology Fusion Review Panel chaired by John Holdren. He argued [Holdren 95]: The options available for meeting the world’s demand for energy in 2050 and beyond are those already in use – fossil fuels, biomass energy, nuclear fission, hydropower, geothermal energy, wind energy, and solar energy – plus, potentially, nuclear fusion. In these circumstances, it should be obvious that there is great merit in the pursuit of diversity in energy options for the next century. There are not so many possibilities altogether. The greater the number of these that can be brought to the point of commercialization, the greater will be the chance that overall energy needs can be met without encountering excessive costs from or unmanageable burdens upon any one source. -
Plasma Physics and Controlled Nuclear Fusion Research 1984 Vol.3 TENTH CONFERENCE PROCEEDINGS, LONDON, 12-19 SEPTEMBER 1984 Nuclear Fusion, Supplement 1985
Plasma Physics and Controlled Nuclear Fusion Research 1984 Vol.3 TENTH CONFERENCE PROCEEDINGS, LONDON, 12-19 SEPTEMBER 1984 Nuclear Fusion, Supplement 1985 fj&\ VW& INTERNATIONAL ATOMIC ENERGY AGENCY, VIENNA, 1985 ^^ m PLASMA PHYSICS AND CONTROLLED NUCLEAR FUSION RESEARCH 1984 VOLUME 3 The following States are Members of the International Atomic Energy Agency: AFGHANISTAN HAITI PARAGUAY ALBANIA HOLY SEE PERU ALGERIA HUNGARY PHILIPPINES ARGENTINA ICELAND POLAND AUSTRALIA INDIA PORTUGAL AUSTRIA INDONESIA QATAR BANGLADESH IRAN, ISLAMIC REPUBLIC OF ROMANIA BELGIUM IRAQ SAUDI ARABIA BOLIVIA IRELAND SENEGAL BRAZIL ISRAEL SIERRA LEONE BULGARIA ITALY SINGAPORE BURMA IVORY COAST SOUTH AFRICA BYELORUSSIAN SOVIET JAMAICA SPAIN SOCIALIST REPUBLIC JAPAN SRI LANKA CAMEROON JORDAN SUDAN CANADA KENYA SWEDEN CHILE KOREA, REPUBLIC OF SWITZERLAND CHINA KUWAIT SYRIAN ARAB REPUBLIC COLOMBIA LEBANON THAILAND COSTA RICA LIBERIA TUNISIA CUBA LIBYAN ARAB JAMAHIRIYA TURKEY CYPRUS LIECHTENSTEIN UGANDA CZECHOSLOVAKIA LUXEMBOURG UKRAINIAN SOVIET SOCIALIST DEMOCRATIC KAMPUCHEA MADAGASCAR REPUBLIC DEMOCRATIC PEOPLE'S MALAYSIA UNION OF SOVIET SOCIALIST REPUBLIC OF KOREA MALI REPUBLICS DENMARK MAURITIUS UNITED ARAB EMIRATES DOMINICAN REPUBLIC MEXICO UNITED KINGDOM OF GREAT ECUADOR MONACO BRITAIN AND NORTHERN EGYPT MONGOLIA IRELAND EL SALVADOR MOROCCO UNITED REPUBLIC OF ETHIOPIA NAMIBIA TANZANIA FINLAND NETHERLANDS UNITED STATES OF AMERICA FRANCE NEW ZEALAND URUGUAY GABON NICARAGUA VENEZUELA GERMAN DEMOCRATIC REPUBLIC NIGER VIET NAM GERMANY, FEDERAL REPUBLIC OF NIGERIA YUGOSLAVIA GHANA NORWAY ZAIRE GREECE PAKISTAN ZAMBIA GUATEMALA PANAMA The Agency's Statute was approved on 23 October 1956 by the Conference on the Statute of the IAEA held at United Nations Headquarters, New York; it entered into force on 29 July 1957. The Headquarters of the Agency are situated in Vienna. -
Feasibility of Inertial-Confinement Fusion
On October 15, 1981, John H. Nuckolls this article has occurred because of the received the American Physical Society's dedication and inspiration of John Maxwell Prize for outstanding contribu Nuckolls and his colleagues at LLNL, as tions to plasma physics. The citation read well as of hundreds of researchers else "For his contributions to the genesis and where in the United States and other na progress of inertial confinement fusion. tions. In addition to their work, consistent His insight into the fundamental physics support for the U.S. Inertial Fusion Pro issues has served to guide and inspire the gram has been provided by the Depart technical evolution of the field." An article ment of Energy and its predecessors and based on his Maxwell lecture to the Soci by the Congress of the United States. This ety was published in Physics Today (Sep support has led, in 10 years time, to an ef tember 1982). Because of the interest that fort with the accomplishments and scope readers of the En ergy and Technol ogy described in this article. It should be fur Review could have in John's views on ther noted that, although the thrust of this John's views on inertial confinement fusion, the editors article is directed toward the long-range power-potential of the En ergy and Technology Review have agreed to re of the Inertial Fusion Program, current support and print the article in this issue. The work described in nearer-term goals are defense related. Feasibility of Inertial Confinement Fusion "We can see no insurmountable roadblocks to th e practi temperatures sufficient to cause the hy cal achievement of electrical power generated by in ertial drogen nuclei to fuse, releasing an confinement fusion .. -
Lawrence Livermore National Laboratory (LLNL)
LLNL Capabilities Relevant to the INFUSE Program Andris Dimits Presented at the INFUSE Workshop Lawrence Livermore National Laboratory Knoxville, TN, November 23, 2019 Email: [email protected] Ph: 925-422-0211 LLNL-PRES-797381 This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under contract DE-AC52-07NA27344. Lawrence Livermore National Security, LLC Outline § LLNL – some background § Organization of LLNL’s fusion-related departments § LLNL’s technical expertise related to fusion — MFE — IFE § Software § Facilities of potential interest for collaboration — User facilities — Other facilities of potential interest § Student intern and university faculty programs 2 LLNL-PRES-797381 LLNL – Some notable facts – (www.llnl.gov/about) § Managed by Lawrence Livermore National Security, LLC for NNSA § ~6,900 employees; ~2,700 scientists and engineers § Established in 1952 on the grounds of the decommissioned Livermore Naval Air Station § Prior to that, second site for UC Radiation Laboratory (Berkeley) — “Materials Testing Accelerator” — Development of diagnostics for nuclear weapons testing § Early involvement in controlled fusion — Magnetic mirrors (R. F. Post experiments, 1952 – MFTF-B, 1987) — Laser-based ICF • Nuckols 1960 – proposed idea of controlled ICF based on computations • Shiva laser 1977 § Wide array of activities in controlled fusion (ICF, MFE), HED sciences, materials sciences and other areas relevant to fusion energy 3 LLNL-PRES-797381 LLNL departments relevant -
Nuclear Diagnostics for Inertial Confinement Fusion (ICF) Plasmas
Plasma Physics and Controlled Fusion TOPICAL REVIEW Nuclear diagnostics for Inertial Confinement Fusion (ICF) plasmas To cite this article: J A Frenje 2020 Plasma Phys. Control. Fusion 62 023001 View the article online for updates and enhancements. This content was downloaded from IP address 18.21.213.6 on 07/01/2020 at 20:53 Plasma Physics and Controlled Fusion Plasma Phys. Control. Fusion 62 (2020) 023001 (44pp) https://doi.org/10.1088/1361-6587/ab5137 Topical Review Nuclear diagnostics for Inertial Confinement Fusion (ICF) plasmas J A Frenje Massachusetts Institute of Technology, Cambridge, MA 02139, United States of America E-mail: [email protected] Received 12 December 2017, revised 13 September 2019 Accepted for publication 25 October 2019 Published 7 January 2020 Abstract The field of nuclear diagnostics for Inertial Confinement Fusion (ICF) is broadly reviewed from its beginning in the seventies to present day. During this time, the sophistication of the ICF facilities and the suite of nuclear diagnostics have substantially evolved, generally a consequence of the efforts and experience gained on previous facilities. As the fusion yields have increased several orders of magnitude during these years, the quality of the nuclear-fusion-product measurements has improved significantly, facilitating an increased level of understanding about the physics governing the nuclear phase of an ICF implosion. The field of ICF has now entered an era where the fusion yields are high enough for nuclear measurements to provide spatial, temporal and spectral information, which have proven indispensable to understanding the performance of an ICF implosion. At the same time, the requirements on the nuclear diagnostics have also become more stringent.