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Environmental Impact Statement and Environmental Impact Report for Continued Operation of Lawrence Livermore National Laboratory and Sandia National Labo
Environmental Impact Statement and Environmental Impact Report for Continued Operation of Lawrence Livermore National Laboratory and Sandia National Labo... APPENDIX A DESCRIPTION OF MAJOR PROGRAMS AND FACILITIES Appendix A describes the programs, infrastructures, facilities, and future plans of Lawrence Livermore National Laboratory (LLNL) and the Sandia National Laboratories at Livermore (SNL, Livermore). It provides information on existing activities and facilities, as well as information on those activities anticipated to occur or facilities to be constructed over the next 5 to 10 years. The purpose of this appendix is to: present information that can be used to evaluate the proposed action and other EIS/EIR alternatives, identify activities that are part of the proposed action, distinguish proposed action activities from no action alternative activities, and provide supporting documentation for less detailed descriptions of these activities or facilities found in other sections and appendices of the EIS/EIR. Figure A-1 illustrates how this appendix interfaces with other sections and appendices of this EIS/EIR. Most LLNL and all SNL, Livermore operations are located at sites near Livermore, California. LLNL also operates LLNL Site 300 near Tracy, California, and conducts limited activities at several leased properties near the LLNL Livermore site, as well as in leased offices in Los Angeles, California, and Germantown, Maryland. Figure A-2 and Figure A-3 show the regional location of the LLNL Livermore site, LLNL Site 300, and SNL, Livermore and their location with respect to the cities of Livermore and Tracy. While they are distinct operations managed and operated by different contractors, for purposes of this document LLNL Livermore and SNL, Livermore sites are addressed together because of their proximity. -
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. -
Laser Fusion Program Overview
Energyand Technology Review Lawrence Livermore Laboratory August 1977 ~ j NATIONAL SECURITY Laser Fusion Program Overview In the last three years, we have witnessed ex with the ultimate goal of generating power from tremely rapid advances in the theoretical and ex controlled thermonuclear reactions. The two major perimental understanding of laser fusion. Our approaches to controlled fusion are magnetic con program is structured to proceed through a series of finement and inertial confinement, both of which well defined fusion milestones to proof of the scientific require heating a deuterium-tritium mixture to an feasibility of laser fusion with the Shiva Nova system. ignition temperature of about 108 K . The magnetic Concurrently, we are studying those key technical confinement technique uses magnetic fields to con areas, such as advanced lasers, which are required to fine a low-density 0-T plasma for the long time re progress beyond proof of feasibility. We have iden quired for efficient burn of the low-density fuel: 10 14 tified and quantified the opportunities and key ions per cm3 confined for a few seconds. rn contrast, technical issues in military applications, such as the inertial confinement fusion process uses laser or weapons effects simulations, and in civilian applica particle beams to compress a small thermonuclear tions, such as central-station electric power produc fuel pellet (target) to between 1000 and 10 000 times tion. In this issue of the Energy and Technology liquid density for an extremely short time (1026 ions Review, we summarize the current status and future per cm 3 for lOps). A t such high densities, the fuel plans for the laser fusion program at LLL, emphasiz burns so rapidly that efficient burn is achieved ing the civilian applications of laser fusion. -
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. -
2Fi Lawrence Livermore Laboratory I*^P^*S
V PREPRINT UCRL- 77944 Ur,\>\--m'>te^-2fi Lawrence Livermore Laboratory STATUS OF LARGE NEODYHIUM GLASS LASERS James A. Glaze, William W. Simmons and Wilhelm F. Hagen March ID, 1976 mm This Paper was Prepared for Submission to the Society of Photo-Optical Instrumentation Engineers SPIE Meeting, Reston, VA March 22-23, 1976 This is a preprint ot a paper intended for publication in a journal or proceedings. Since changes may be made before publication, this preprint is made available with the understanding that it will not be cited or reproduced without the permission of the author. i*^P^*S' ««*- -»v«>*^_ DiSTRiKUTiONC; 7602 STATUS OF LARGE NEODYMIUM GLASS LASERS* •ponum] by llw Van* Stu „ o| M[l Blmc*i ng PttritrmtM A« Canes A. Glaje, William H. Simmons and Wlhelm F. Hagen uitKnnmtion. 01 IIKU tiqitiqRt, Laser Fusion Division, Lawrence Livermore Laboratory nmnir. <ieir» 01 tngfttd Llvermore, California 94550 *IR£t» ottTIfcnitttllly f.tth mrnw en>,«l* owned (HJHi. Introduction The Nd:Glass laser is used extensively throughout the world for laser fusion and laser plasma Inter action studies. Its popularity, to a large extent, stems from the fact that 1t 1s capable of operating reliably in the subnanosecond-terawatt power regime. In addition, the technology necessary to combine a large number of laser chains to produce a system capable of multi-terawatt performance currently exists and is being applied. At the Lawrence Livermore Laboratory two large laser systems are currently in operation and two are under construction. The OANUS and CYCLOPS systems produce 0.5 and 1 terawatt of focusable power 1n 0.1 ns respectively. -
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 -
The Project Gutenberg Ebook of Project Cyclops, by Thomas Hoover
The Project Gutenberg EBook of Project Cyclops, by Thomas Hoover This eBook is for the use of anyone anywhere at no cost and with almost no restrictions whatsoever. You may copy it, give it away or re-use it under the terms of the Project Gutenberg License included with this eBook or online at www.gutenberg.org ** This is a COPYRIGHTED Project Gutenberg eBook, Details Below ** ** Please follow the copyright guidelines in this file. ** Title: Project Cyclops Author: Thomas Hoover Release Date: November 14, 2010 [EBook #34319] Language: English Character set encoding: UTF-8 *** START OF THIS PROJECT GUTENBERG EBOOK PROJECT CYCLOPS *** Produced by Al Haines ============================================================== This work is licensed under a Creative Commons Attribution 3.0 Unported License, http://creativecommons.org/ ============================================================== THOMAS HOOVER “A high-tech launch site, a missing nuke, and Arab terrorists with nothing to lose . .” In the sun-dappled waters of the Aegean, ex-agent Michael Vance pilots the Odyssey II, a handmade replica of the sailcraft of the ancient hero Ulysses. Out of nowhere, a Russian Hind gunship with Arab terrorists at the helm fires upon the tiny ship below. The terrorists’ destination is a tiny Aegean island where a U.S. aerospace corporation carefully guards the Cyclops 20-megawatt laser launch facility. But the company security force is no match for the firepower of the Arab invasion and the launch site is quickly overrun. With helpless horror, the executives can only watch as renegade technicians convert the launch vehicle into a ballistic missile that can deliver their stolen thermonuclear warhead to any city in the U.S. -
Fusion Reactions
Nuclear Fusion Technology Dr. BC Choudhary, Professor Applied Science Department, NITTTR, Sector-26, Chandigarh-160019. Content Outlines Review of Nuclear Processes Nuclear Fusion Reactions Fusion Reactor Technologies Technological Developments Pros and Cons Foreseeable trends Four Forces of Nature Systematic Information about Nucleus . Nuclear density at the centre of the nucleus 44 3 0 10 nucleons/m Density of nucleons (r) in the inner region of the nucleus is about same for all nuclei. Surface thickness of all nuclei are very similar 1/3 Radius of nucleus, R = R0 A , small variation in radii . NOT ALL NUCLEI ARE SPHERICAL. Energies of nucleons in nucleus 10 MeV . ALL NUCLEI ARE NOT STABLE Nuclear Stability Proton unstable Stable nuclei Neutron unstable Stable n:p = 1.2 –1.4 Measure of Nuclear Stability . Binding Energy per nucleon 2 EB(Z,N) = {ZMp+NMn - M(Z,N)} c • Nuclei with the largest binding energy per nucleon are the most stable. • The largest binding energy per nucleon is 8.7 MeV, for mass number A = 60. • Beyond Bismuth, A = 209, nuclei are unstable. Nuclear Processes . We can release energy by creating nuclei that are more strongly bound (increasing Eb) Fission: Heaviest nuclei 56 Eb Fe split into smaller fragments. 238 N U Fusion: Lightest nuclei 1H combine to form heavier N nuclei. Both the processes evolve large amount of energy. Nuclear Fission and Fusion Nuclear fission: A large nucleus splits into several small nuclei when impacted by a neutron, and energy is released in this process Nuclear fusion: Several small nuclei fuse together and release energy Electricity from Nuclear Fission Nuclear power plants account ~17 percent of the worlds power. -
Fusion Devices
PP.EPRINI UCRL-S0060 r~ _ _ZZ~ j Lawrence Uvermore Laboratory FUSION DEVICES T. K. FOWLER OCTOBER 11, 197"/ Presented at the EPRI Executive Seminar on Fusion, October 11-13, 1977 San Francisco, California This is a preprint of a paper intended for publication in a Journal or proceedings. Since changes may be made before publication, this preprint is made available with the understanding that It will not be cited or reproduced without the permission of the author. )0B ©1STR1BUT10N OF THIS DOCUMENT IS UNLIMITED 1. FUSION DEVICES T. K. Fowler In this talk, I will emphasize the expected developments in fusion research over the next five years. This will be the formative period for fusion in the foreseeable future. It will also be a formative period in national energy policy that will impact many years to come. As the previous speakers have said, we believe that fusion is a matter of great interest to the electric utilities. We need your support and your guidance in this critically formative period. I will give a brief description of the three mainline activities of the research program in fusion. These include two magnetic systems, one called the Tokamak and one called the mirror machine, and also laser fusion. While I am going to concentrate on these three mainline activities, they are not the only possibilities. Fusion is a rich subject with many possible outcomes, all of which may be interesting to the utilities. However, the first ways that fusion will be made practical will, I think, come from the approaches I will describe, simply because each of these concepts already has behind it a long history of scientific development that should culminate in the next five years. -
Beam-Propagation Studies on Cyclops
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 BEAM-PROPAGATION STUDIES ON CYCLOPS -------------------- Cyclops, a single-chain Nd :glass laser, produces a Cyclops Laser Chain I-TW sub nanosecond pulse whose brightness exceeds The Cyclops laser chain is shown schematically in 1018 W/cm 2 ·sr. This is state-of-the-art performance Fig . 14. The dye-mode-locked Nd: Y AG oscillator with for solid-state laser technology. Three key factors have its optically triggered sp ark-gap switchout produces a contributed to this achievement: disk amplifiers in the Single 1.5 -m 1, 100-ps pulse of 1.06-J1m light. This pulse final power stage with 20-cm clear apertures, spatial is amplified by two stages of rod preamplifiers and filters for controlling small-scale self-focusing, and three stages of disk amplifiers. The basic staging after quadratic apertures for mmlmlzmg whole-beam initial preamplification includes an iteration of distortion. Cyclops serves both as a prototype for multilayer dielectric-coated polarizers, pulsed Faraday future multiarmed laser systems and as a full-scale rotators, and amplifiers. The rotator-polarizer experimental amplifier facility for investigating combinations provide about 25 dB of backward beam-propagation phenomena and testing system attenuation for each 10 dB of gain in the forward components. direction. This ensures that laser components will not A number of laboratories throughout the world are be damaged as a result of target reflections.