A. Nobile
Los Alamos National Laboratory
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Featured researches published by A. Nobile.
Physics of Plasmas | 2009
H. W. Herrmann; James R. Langenbrunner; J. M. Mack; J.H. Cooley; D. C. Wilson; S. C. Evans; T. J. Sedillo; G. A. Kyrala; S. E. Caldwell; C. S. Young; A. Nobile; Joseph R. Wermer; Stephen N. Paglieri; A. McEvoy; Y. Kim; S. H. Batha; C. J. Horsfield; D.W. Drew; Warren Garbett; M. S. Rubery; V. Yu. Glebov; S. Roberts; J. A. Frenje
Glass capsules were imploded in direct drive on the OMEGA laser [Boehly et al., Opt. Commun. 133, 495 (1997)] to look for anomalous degradation in deuterium/tritium (DT) yield and changes in reaction history with H3e addition. Such anomalies have previously been reported for D/H3e plasmas but had not yet been investigated for DT/H3e. Anomalies such as these provide fertile ground for furthering our physics understanding of inertial confinement fusion implosions and capsule performance. Anomalous degradation in the compression component of yield was observed, consistent with the “factor of 2” degradation previously reported by Massachusetts Institute of Technology (MIT) at a 50% H3e atom fraction in D2 using plastic capsules [Rygg, Phys. Plasmas 13, 052702 (2006)]. However, clean calculations (i.e., no fuel-shell mixing) predict the shock component of yield quite well, contrary to the result reported by MIT but consistent with Los Alamos National Laboratory results in D2/H3e [Wilson et al., J. Phys.: Conf....
Physics of Plasmas | 2004
R. E. Olson; R. J. Leeper; A. Nobile; John A. Oertel; Gordon Andrew Chandler; K. Cochrane; S. C. Dropinski; S. C. Evans; S. W. Haan; J. L. Kaae; J. P. Knauer; K. Lash; L. P. Mix; A. Nikroo; G. A. Rochau; G. Rivera; C. Russell; Diana Grace Schroen; R. J. Sebring; D. L. Tanner; R. E. Turner; R. J. Wallace
The velocities and temperatures of shock waves generated by laser-driven hohlraum radiation fields have been measured in indirect-drive inertial confinement fusion (ICF) capsule ablator materials. Time-resolved measurements of the preheat temperature ahead of the shock front have been performed and included in the analysis. Measurements of the x-ray burnthrough of the ablation front and the ablator x-ray re-emission have also been made in the Cu-doped beryllium, polyimide, and Ge-doped CH ablator samples. The experiments utilize 15 beams of the University of Rochester Omega Laser [Soures et al., Phys. Plasmas 3, 2108 (1996)] to heat hohlraums to radiation temperatures of ∼120–200 eV. In the experiments, planar samples of ablator material are exposed to the hohlraum radiation field, generating shocks in the range of 10–50 Mbars. The experimental results are compared to integrated two-dimensional Lasnex [G. B. Zimmerman and W. L. Kruer, Comments Plasma Phys. Control. Fusion 2, 51 (1975)] calculations, in wh...
Laser and Particle Beams | 2006
A. Nobile; A. Nikroo; Robert Cook; J.C. Cooley; D.J. Alexander; R.E. Hackenberg; C.T. Necker; R.M. Dickerson; J.L. Kilkenny; T.P. Bernat; K. C. Chen; H. Xu; R. Stephens; H. Huang; S.W. Haan; A.C. Forsman; L.J. Atherton; S. Letts; M.J. Bono; Douglas Wilson
An important component of the U.S. effort to achieve thermonuclear ignition in 2010 on the National Ignition Facility is the development of high quality 2 mm diameter spherical capsules to function as the ablator and contain the cryogenic DT fuel. Three ignition capsule designs have been developed, and detailed fabrication specifications for each design have been established and placed under change control. A research program with activities coordinated mainly between Lawrence Livermore, General Atomics and Los Alamos is underway to demonstrate fabrication of capsules meeting specifications. The point design for ignition campaigns beginning in 2010 is a Cu-doped Be capsule that has a radial gradient in Cu dopant level in the capsule wall. This capsule is being produced by sputter deposition of Be and Cu onto either a hollow glow discharge polymer (GDP) spherical mandrel or a solid spherical mandrel, followed by removal of the mandrel and polishing of the capsule. A key goal in the U.S. is to demonstrate fabrication of this capsule by the end of 2006. Two other ignition capsule designs are also being developed as contingencies to the point design. One contingency design is a GDP capsule that has a radial Ge dopant level in its wall. This capsule is produced by co-deposition of Ge and GDP onto a PAMS mandrel followed by thermal removal of the mandrel. The second contingency design is a uniform Cu-doped Be capsule that is fabricated from high purity fine grain Be0.3at.%Cu alloy using a precision machining route followed by polishing. Ignition targets to be fielded in 2010 will be filled with DT fuel through a small fill hole. Laser drilling capability has been developed and used to drill approximately 5 μm diameter holes through capsule walls for DT filling. Characterization methods necessary for characterizing capsules are being developed.
Laser and Particle Beams | 2005
J.D. Kilkenny; N.B. Alexander; A. Nikroo; D.A. Steinman; A. Nobile; T.P. Bernat; Robert Cook; S. Letts; M. Takagi; D. R. Harding
Success in inertial confinement fusion (ICF) requires sophisticated, characterized targets. The increasing fidelity of three-dimensional (3D), radiation hydrodynamic computer codes has made it possible to design targets for ICF which can compensate for limitations in the existing single shot laser and Z pinch ICF drivers. Developments in ICF target fabrication technology allow more esoteric target designs to be fabricated. At present, requirements require new deterministic nano-material fabrication on micro scale.
Nuclear Fusion | 2004
D. T. Goodin; N.B. Alexander; L.C. Brown; D.T. Frey; R. Gallix; C. R. Gibson; J.L. Maxwell; A. Nobile; C.L. Olson; R. Raffray; Gary Eugene Rochau; D. G. Schroen; M. S. Tillack; W.S. Rickman; B. A. Vermillion
A central feature of an inertial fusion energy (IFE) power plant is a target that has been compressed and heated to fusion conditions by the energy input of the driver. This is true whether the driver is a laser system, heavy ion beams or Z-pinch system. The IFE target fabrication, injection and tracking programmes are focusing on methods that will scale to mass production. We are working closely with target designers, and power plant systems specialists, to make specifications and material selections that will satisfy a wide range of required and desirable target characteristics. One-of-a-kind capsules produced for today’s inertial confinement fusion experiments are estimated to cost about US
Fusion Science and Technology | 2003
Warren P. Steckle; A. Nobile
2500 each. Design studies of cost-effective power production from laser and heavy-ion driven IFE have suggested a cost goal of about
Fusion Science and Technology | 2005
D. T. Goodin; N.B. Alexander; L.C. Brown; D. A. Callahan; Peter S. Ebey; D.T. Frey; R. Gallix; Drew A. Geller; C. R. Gibson; James K. Hoffer; J.L. Maxwell; Barry McQuillan; A. Nikroo; A. Nobile; C.L. Olson; R. Raffray; W.S. Rickman; Gary Eugene Rochau; D. G. Schroen; J. D. Sethian; John D. Sheliak; J. Streit; M. S. Tillack; B. A. Vermillion; E.I. Valmianski
0.25–0.30 for each injected target (corresponding to ∼10% of the ‘electricity value’ in a target). While a four orders of magnitude cost reduction may seem at first to be nearly impossible, there are many factors that suggest this is achievable. This paper summarizes the design, specifications, requirements and proposed manufacturing processes for the future for laser fusion, heavy ion fusion and Z-pinch driven targets. These target manufacturing processes have been developed—and are proposed—based on the unique materials science and technology programmes that are ongoing for each of the target concepts. We describe the paradigm shifts in target manufacturing methodologies that will be needed to achieve orders of magnitude reductions in target costs, and summarize the results of ‘nth-of-a-kind’ plant layouts and cost estimates for future IFE power plant fuelling. These engineering studies estimate the cost of the target supply in a fusion economy, and show that costs are within the range of commercial feasibility for electricity production.
Fusion Science and Technology | 2003
Ana M. Schwendt; A. Nobile; Peter L. Gobby; Warren P. Steckle; Denis G. Colombant; J. D. Sethian; D. T. Goodin; G. E. Besenbruch
Low-density polymer foams have been an integral part of targets used in inertial confinement fusion (ICF) experiments. Target designs are unique in the ICF program, and targets are made on an individual basis. Costs for these targets are high due to the time required to machine, assemble, and characterize each target. To produce targets in high volume and at low cost, a polymer system is required that is amenable to scale up. High internal phase emulsion (HIPE) polystyrene is a robust system that offers great flexibility in terms of tailoring the density and incorporating metal dopants. Emulsions used to fabricate HIPE foams currently are made in a batch process. With the use of metering pumps for both the water and oil phases, emulsions can be produced in a continuous process. This not only makes these foams potential candidates for direct-drive capsules, but high-Z dopants can be metered in making these foams attractive for hohlraum components in indirect-drive systems. Preparation of HIPE foams are discussed for both direct-drive and indirect-drive systems.
Laser and Particle Beams | 2002
D. T. Goodin; A. Nobile; N.B. Alexander; L.C. Brown; J.L. Maxwell; J. Pulsifer; A.M. Schwendt; M. S. Tillack; R.S. Willms
Abstract A central feature of an Inertial Fusion Energy (IFE) power plant is a target that has been compressed and heated to fusion conditions by the energy input of the driver. The technology to economically manufacture and then position cryogenic targets at chamber center is at the heart of future IFE power plants. For direct drive IFE (laser fusion), energy is applied directly to the surface of a spherical CH polymer capsule containing the deuterium-tritium (DT) fusion fuel at approximately 18K. For indirect drive (heavy ion fusion, HIF), the target consists of a similar fuel capsule within a cylindrical metal container or ’’hohlraum’’ which converts the incident driver energy into x-rays to implode the capsule. For either target, it must be accurately delivered to the target chamber center at a rate of about 5-10Hz, with a precisely predicted target location. Future successful fabrication and injection systems must operate at the low cost required for energy production (about
Fusion Science and Technology | 2004
W. P. Steckle; M. E. Smith; R. J. Sebring; A. Nobile
0.25/target, about 104 less than current costs). Z-pinch driven IFE (ZFE) utilizes high current pulses to compress plasma to produce x-rays that indirectly heat a fusion capsule. ZFE target technologies utilize a repetition rate of about 0.1 Hz with a higher yield. This paper provides an overview of the proposed target methodologies for laser fusion, HIF, and ZFE, and summarizes advances in the unique materials science and technology development programs.