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Dive into the research topics where Thomas James Awe is active.

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Featured researches published by Thomas James Awe.


Physics of Plasmas | 2014

Modified helix-like instability structure on imploding z-pinch liners that are pre-imposed with a uniform axial magnetic field.

Thomas James Awe; Christopher A. Jennings; R. D. McBride; M. E. Cuneo; Derek C. Lamppa; M. R. Martin; Dean C. Rovang; Daniel Brian Sinars; Stephen A. Slutz; A. C. Owen; Kurt Tomlinson; M. R. Gomez; Stephanie B. Hansen; Mark Herrmann; M. Jones; J. L. McKenney; G. K. Robertson; G. A. Rochau; M. E. Savage; D. G. Schroen; W. A. Stygar

Recent experiments at the Sandia National Laboratories Z Facility have, for the first time, studied the implosion dynamics of magnetized liner inertial fusion (MagLIF) style liners that were pre-imposed with a uniform axial magnetic field. As reported [T. J. Awe et al., Phys. Rev. Lett. 111, 235005 (2013)] when premagnetized with a 7 or 10 T axial field, these liners developed 3D-helix-like hydrodynamic instabilities; such instabilities starkly contrast with the azimuthally correlated magneto-Rayleigh-Taylor (MRT) instabilities that have been consistently observed in many earlier non-premagnetized experiments. The helical structure persisted throughout the implosion, even though the azimuthal drive field greatly exceeded the expected axial field at the liners outer wall for all but the earliest stages of the experiment. Whether this modified instability structure has practical importance for magneto-inertial fusion concepts depends primarily on whether the modified instability structure is more stable th...


Physics of Plasmas | 2015

Demonstration of thermonuclear conditions in magnetized liner inertial fusion experimentsa)

M. R. Gomez; Stephen A. Slutz; Adam B Sefkow; Kelly Hahn; Stephanie B. Hansen; P. F. Knapp; Paul Schmit; C. L. Ruiz; Daniel Brian Sinars; Eric Harding; Christopher A. Jennings; Thomas James Awe; Matthias Geissel; Dean C. Rovang; I. C. Smith; Gordon Andrew Chandler; G. W. Cooper; Michael Edward Cuneo; A. J. Harvey-Thompson; Mark Herrmann; Mark Hess; Derek C. Lamppa; M. R. Martin; R. D. McBride; Kyle Peterson; John L. Porter; Gregory A. Rochau; M. E. Savage; D. G. Schroen; W. A. Stygar

The magnetized liner inertial fusion concept [S. A. Slutz et al., Phys. Plasmas 17, 056303 (2010)] utilizes a magnetic field and laser heating to relax the pressure requirements of inertial confinement fusion. The first experiments to test the concept [M. R. Gomez et al., Phys. Rev. Lett. 113, 155003 (2014)] were conducted utilizing the 19 MA, 100 ns Z machine, the 2.5 kJ, 1 TW Z Beamlet laser, and the 10 T Applied B-field on Z system. Despite an estimated implosion velocity of only 70 km/s in these experiments, electron and ion temperatures at stagnation were as high as 3 keV, and thermonuclear deuterium-deuterium neutron yields up to 2 × 1012 have been produced. X-ray emission from the fuel at stagnation had widths ranging from 50 to 110 μm over a roughly 80% of the axial extent of the target (6–8 mm) and lasted approximately 2 ns. X-ray yields from these experiments are consistent with a stagnation density of the hot fuel equal to 0.2–0.4 g/cm3. In these experiments, up to 5 × 1010 secondary deuterium-...


Physical Review Letters | 2016

Experimental Demonstration of the Stabilizing Effect of Dielectric Coatings on Magnetically Accelerated Imploding Metallic Liners.

Thomas James Awe; Kyle Peterson; E. P. Yu; R. D. McBride; Daniel Brian Sinars; M. R. Gomez; Christopher A. Jennings; M. R. Martin; S. E. Rosenthal; D. G. Schroen; Adam B Sefkow; Stephen A. Slutz; Kurt Tomlinson; Roger Alan Vesey

Enhanced implosion stability has been experimentally demonstrated for magnetically accelerated liners that are coated with 70  μm of dielectric. The dielectric tamps liner-mass redistribution from electrothermal instabilities and also buffers coupling of the drive magnetic field to the magneto-Rayleigh-Taylor instability. A dielectric-coated and axially premagnetized beryllium liner was radiographed at a convergence ratio [CR=Rin,0/Rin(z,t)] of 20, which is the highest CR ever directly observed for a strengthless magnetically driven liner. The inner-wall radius Rin(z,t) displayed unprecedented uniformity, varying from 95 to 130  μm over the 4.0 mm axial height captured by the radiograph.


Review of Scientific Instruments | 2014

Pulsed-coil magnet systems for applying uniform 10–30 T fields to centimeter-scale targets on Sandia's Z facility

Dean C. Rovang; Derek C. Lamppa; M. E. Cuneo; Albert C. Owen; J. L. McKenney; Drew Johnson; S. Radovich; R. J. Kaye; R. D. McBride; C. S. Alexander; Thomas James Awe; Stephen A. Slutz; Adam B Sefkow; Thomas A. Haill; P. A. Jones; J. W. Argo; D. G. Dalton; G. K. Robertson; E.M. Waisman; Daniel Brian Sinars; J. Meissner; M. Milhous; D. N. Nguyen; C. H. Mielke

Sandia has successfully integrated the capability to apply uniform, high magnetic fields (10-30 T) to high energy density experiments on the Z facility. This system uses an 8-mF, 15-kV capacitor bank to drive large-bore (5 cm diameter), high-inductance (1-3 mH) multi-turn, multi-layer electromagnets that slowly magnetize the conductive targets used on Z over several milliseconds (time to peak field of 2-7 ms). This system was commissioned in February 2013 and has been used successfully to magnetize more than 30 experiments up to 10 T that have produced exciting and surprising physics results. These experiments used split-magnet topologies to maintain diagnostic lines of sight to the target. We describe the design, integration, and operation of the pulsed coil system into the challenging and harsh environment of the Z Machine. We also describe our plans and designs for achieving fields up to 20 T with a reduced-gap split-magnet configuration, and up to 30 T with a solid magnet configuration in pursuit of the Magnetized Liner Inertial Fusion concept.


Physics of Plasmas | 2015

Diagnosing magnetized liner inertial fusion experiments on Za)

Stephanie B. Hansen; M. R. Gomez; Adam B Sefkow; Stephen A. Slutz; Daniel Brian Sinars; Kelly Hahn; Eric Harding; P. F. Knapp; Paul Schmit; Thomas James Awe; R. D. McBride; Christopher A. Jennings; Matthias Geissel; A. J. Harvey-Thompson; Kyle Peterson; Dean C. Rovang; Gordon Andrew Chandler; G. W. Cooper; Michael Edward Cuneo; Mark Herrmann; Mark Hess; Owen Johns; Derek C. Lamppa; M. R. Martin; John L. Porter; G. K. Robertson; G. A. Rochau; C. L. Ruiz; M. E. Savage; I. C. Smith

Magnetized Liner Inertial Fusion experiments performed at Sandias Z facility have demonstrated significant thermonuclear fusion neutron yields (∼1012 DD neutrons) from multi-keV deuterium plasmas inertially confined by slow (∼10 cm/μs), stable, cylindrical implosions. Effective magnetic confinement of charged fusion reactants and products is signaled by high secondary DT neutron yields above 1010. Analysis of extensive power, imaging, and spectroscopic x-ray measurements provides a detailed picture of ∼3 keV temperatures, 0.3 g/cm3 densities, gradients, and mix in the fuel and liner over the 1–2 ns stagnation duration.


Physics of Plasmas | 2016

Exploring magnetized liner inertial fusion with a semi-analytic model

R. D. McBride; Stephen A. Slutz; Roger A. Vesey; M. R. Gomez; Adam B Sefkow; Stephanie B. Hansen; P. F. Knapp; Paul Schmit; Matthias Geissel; A. J. Harvey-Thompson; Christopher A. Jennings; Eric Harding; Thomas James Awe; Dean C. Rovang; Kelly Hahn; M. R. Martin; Kyle Robert Cochrane; Kyle Peterson; Gregory A. Rochau; John L. Porter; W. A. Stygar; Edward Michael Campbell; Charles Nakhleh; Mark Herrmann; Michael Edward Cuneo; Daniel Brian Sinars

In this paper, we explore magnetized liner inertial fusion (MagLIF) [S. A. Slutz et al., Phys. Plasmas 17, 056303 (2010)] using a semi-analytic model [R. D. McBride and S. A. Slutz, Phys. Plasmas 22, 052708 (2015)]. Specifically, we present simulation results from this model that: (a) illustrate the parameter space, energetics, and overall system efficiencies of MagLIF; (b) demonstrate the dependence of radiative loss rates on the radial fraction of the fuel that is preheated; (c) explore some of the recent experimental results of the MagLIF program at Sandia National Laboratories [M. R. Gomez et al., Phys. Rev. Lett. 113, 155003 (2014)]; (d) highlight the experimental challenges presently facing the MagLIF program; and (e) demonstrate how increases to the preheat energy, fuel density, axial magnetic field, and drive current could affect future MagLIF performance.


ieee international pulsed power conference | 2009

Numerical simulations of thick aluminum wire behavior under megaampere current drive

Sergey F. Garanin; Sergey D. Kuznetsov; W.L. Atchison; R.E. Reinovsky; Thomas James Awe; Bruno S. Bauer; S. Fuelling; Irvin R. Lindemuth; Richard E. Siemon

A series of experiments to study the behavior of thick wires (0.5-2 mm in diameter) driven by currents of about 1 MA has recently been conducted on the Zebra facility at the University of Nevada, Reno. The objective of these experiments was to study plasma formation on the surface of conductors under the influence of megagauss magnetic fields. Laser shadowgraphy, filtered optical and extreme ultraviolet photodiodes, and extreme ultraviolet spectroscopy used in the experiments provided data on radial expansion of wires and on plasma radiation. This paper focuses on numerical simulations of these experiments. Simulations with wires having diameters up to 1.6 mm demonstrated plasma formation with temperatures above 3 eV, which is in preliminary agreement with the experiment. For 2-mm-diameter wires, although plasma can be observed in the simulations, it has substantially smaller optical thickness than in the simulations of the smaller diameter wires, and the radiation fluxes prove to be much lower. This can shed light on the experimental results where the radiation of the 2-mm wires was very weak. The simulated time dependences of the wire radii agree rather well with the experimental results obtained using laser diagnostics and visible-light imaging. The experimental data of the photodiodes also agree well with the simulated time dependence of the detected radiation.


Physics of Plasmas | 2017

Auto-magnetizing liners for magnetized inertial fusion

Stephen A. Slutz; Christopher A. Jennings; Thomas James Awe; Gabriel Shipley; Brian Thomas Hutsel; Derek C. Lamppa

The MagLIF (Magnetized Liner Inertial Fusion) concept [Slutz et al., Phys. Plasmas 17, 056303 (2010)] has demonstrated fusion-relevant plasma conditions [Gomez et al., Phys. Rev. Lett. 113, 155003 (2014)] on the Z accelerator using external field coils to magnetize the fuel before compression. We present a novel concept (AutoMag), which uses a composite liner with helical conduction paths separated by insulating material to provide fuel magnetization from the early part of the drive current, which by design rises slowly enough to avoid electrical breakdown of the insulators. Once the magnetization field is established, the drive current rises more quickly, which causes the insulators to break down allowing the drive current to follow an axial path and implode the liner in the conventional z-pinch manner. There are two important advantages to AutoMag over external field coils for the operation of MagLIF. Low inductance magnetically insulated power feeds can be used to increase the drive current, and AutoMa...


Physics of Plasmas | 2015

Effects of magnetization on fusion product trapping and secondary neutron spectraa)

P. F. Knapp; Paul Schmit; Stephanie B. Hansen; M. R. Gomez; Kelly Hahn; Daniel Brian Sinars; Kyle Peterson; Stephen A. Slutz; Adam B Sefkow; Thomas James Awe; Eric Harding; Christopher A. Jennings; Michael P. Desjarlais; Gordon Andrew Chandler; G. W. Cooper; Michael Edward Cuneo; Matthias Geissel; A. J. Harvey-Thompson; John L. Porter; Gregory A. Rochau; Dean C. Rovang; C. L. Ruiz; M. E. Savage; Ian Craig Smith; W. A. Stygar; Mark Herrmann

By magnetizing the fusion fuel in inertial confinement fusion (ICF) systems, the required stagnation pressure and density can be relaxed dramatically. This happens because the magnetic field insulates the hot fuel from the cold pusher and traps the charged fusion burn products. This trapping allows the burn products to deposit their energy in the fuel, facilitating plasma self-heating. Here, we report on a comprehensive theory of this trapping in a cylindrical DD plasma magnetized with a purely axial magnetic field. Using this theory, we are able to show that the secondary fusion reactions can be used to infer the magnetic field-radius product, BR, during fusion burn. This parameter, not ρR, is the primary confinement parameter in magnetized ICF. Using this method, we analyze data from recent Magnetized Liner Inertial Fusion experiments conducted on the Z machine at Sandia National Laboratories. We show that in these experiments BR ≈ 0.34(+0.14/−0.06) MG · cm, a ∼ 14× increase in BR from the initial value, and confirming that the DD-fusion tritons are magnetized at stagnation. This is the first experimental verification of charged burn product magnetization facilitated by compression of an initial seed magnetic flux.


Physics of Plasmas | 2011

Bounce-free spherical hydrodynamic implosion

Grigory Kagan; Xianzhu Tang; Scott Hsu; Thomas James Awe

In a bounce-free spherical hydrodynamic implosion, the post-stagnation hot core plasma does not expand against the imploding flow. Such an implosion scheme has the advantage of improving the dwell time of the burning fuel, resulting in a higher fusion burn-up fraction. The existence of bounce-free spherical implosions is demonstrated by explicitly constructing a family of self-similar solutions to the spherically symmetric ideal hydrodynamic equations. When applied to a specific example of plasma liner driven magneto-inertial fusion, the bounce-free solution is found to produce at least a factor of four improvement in dwell time and fusion energy gain.

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Daniel Brian Sinars

Sandia National Laboratories

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M. R. Gomez

Sandia National Laboratories

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Stephen A. Slutz

Sandia National Laboratories

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Kyle Peterson

Sandia National Laboratories

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Stephanie B. Hansen

Sandia National Laboratories

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Adam B Sefkow

Sandia National Laboratories

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P. F. Knapp

Sandia National Laboratories

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R. D. McBride

Sandia National Laboratories

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Eric Harding

Sandia National Laboratories

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