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Featured researches published by A. von Halle.


Physics of Plasmas | 1996

Enhancement of Tokamak Fusion Test Reactor performance by lithium conditioning

D.K. Mansfield; K. W. Hill; J. D. Strachan; M.G. Bell; Stacey D. Scott; R. V. Budny; E. S. Marmar; J. A. Snipes; J. L. Terry; S. H. Batha; R.E. Bell; M. Bitter; C. E. Bush; Z. Chang; D. S. Darrow; D. Ernst; E.D. Fredrickson; B. Grek; H. W. Herrmann; A. Janos; D. L. Jassby; F. C. Jobes; D.W. Johnson; L. C. Johnson; F. M. Levinton; D. R. Mikkelsen; D. Mueller; D. K. Owens; H. Park; A. T. Ramsey

Wall conditioning in the Tokamak Fusion Test Reactor (TFTR) [K. M. McGuire et al., Phys. Plasmas 2, 2176 (1995)] by injection of lithium pellets into the plasma has resulted in large improvements in deuterium–tritium fusion power production (up to 10.7 MW), the Lawson triple product (up to 1021 m−3 s keV), and energy confinement time (up to 330 ms). The maximum plasma current for access to high‐performance supershots has been increased from 1.9 to 2.7 MA, leading to stable operation at plasma stored energy values greater than 5 MJ. The amount of lithium on the limiter and the effectiveness of its action are maximized through (1) distributing the Li over the limiter surface by injection of four Li pellets into Ohmic plasmas of increasing major and minor radius, and (2) injection of four Li pellets into the Ohmic phase of supershot discharges before neutral‐beam heating is begun.


Journal of Vacuum Science and Technology | 1996

Measurements of tritium retention and removal on the Tokamak Fusion Test Reactor

C. H. Skinner; W. Blanchard; J.H. Kamperschroer; P. LaMarche; D. Mueller; A. Nagy; Stacey D. Scott; George Ascione; E. Amarescu; R. Camp; M. Casey; J. Collins; M. Cropper; Charles A. Gentile; M. Gibson; J. C. Hosea; M. Kalish; J. Langford; S.W. Langish; R. Mika; D. K. Owens; G. Pearson; S. Raftopoulos; R. Raucci; T. Stevenson; A. von Halle; D. Voorhees; T. Walters; J. Winston

Recent experiments on the Tokamak Fusion Test Reactor have afforded an opportunity to measure the retention of tritium in a graphite limiter that is subject to erosion, codeposition, and high neutron flux. The tritium was injected by both gas puff and neutral beams. The isotopic mix of hydrogenic recycling was measured spectroscopically and the tritium fraction T/(H+D+T) transiently increased to as high as 75%. Some tritium was pumped out during the experimental run and some removed in a subsequent campaign using various clean‐up techniques. While the short term retention of tritium was high, various conditioning techniques were successful in removing ≊8000 Ci and restoring the tritium inventory to a level well below the administrative limit.


Physics of Plasmas | 1995

Enhanced performance of deuterium--tritium-fueled supershots using extensive lithium conditioning in the Tokamak Fusion Test Reactor

D.K. Mansfield; J. D. Strachan; M.G. Bell; Stacey D. Scott; R.V. Budny; E. S. Marmar; J. A. Snipes; J. L. Terry; S. H. Batha; R. E. Bell; M. Bitter; C.E. Bush; Z. Chang; D. S. Darrow; D. Ernst; E. D. Fredrickson; B. Grek; H. W. Herrmann; K. W. Hill; A. Janos; D.L. Jassby; F. Jobes; D. Johnson; L. C. Johnson; F. W. Levinton; David Mikkelsen; D. Mueller; D. K. Owens; H.K. Park; A. T. Ramsey

In the Tokamak Fusion Test Reactor (TFTR) [K. M. McGuire et al., Phys. Plasmas 2, 2176 (1995)] a substantial improvement in fusion performance has been realized by combining the enhanced confinement due to tritium fueling with the enhanced confinement due to extensive conditioning of the limiter with lithium. This combination has resulted in not only significantly higher global energy confinement times than have previously been obtained in high current supershots, but also in the highest central ratio of thermonuclear fusion output power to input power observed to date.


Physics of Plasmas | 2006

Effect of plasma shaping on performance in the National Spherical Torus Experiment

D.A. Gates; R. Maingi; J. Menard; S.M. Kaye; S.A. Sabbagh; G. Taylor; J. R. Wilson; M.G. Bell; R. E. Bell; S. Bernabei; J. Bialek; T. M. Biewer; W. Blanchard; J.A. Boedo; C.E. Bush; Mark Dwain Carter; Wonho Choe; N.A. Crocker; D. S. Darrow; W. Davis; L. Delgado-Aparicio; S. Diem; J.R. Ferron; A. R. Field; J. Foley; E. D. Fredrickson; R. W. Harvey; Ron Hatcher; W.W. Heidbrink; K. W. Hill

The National Spherical Torus Experiment (NSTX) has explored the effects of shaping on plasma performance as determined by many diverse topics including the stability of global magnetohydrodynamic (MHD) modes (e.g., ideal external kinks and resistive wall modes), edge localized modes (ELMs), bootstrap current drive, divertor flux expansion, and heat transport. Improved shaping capability has been crucial to achieving βt∼40%. Precise plasma shape control has been achieved on NSTX using real-time equilibrium reconstruction. NSTX has simultaneously achieved elongation κ∼2.8 and triangularity δ∼0.8. Ideal MHD theory predicts increased stability at high values of shaping factor S≡q95Ip∕(aBt), which has been observed at large values of the S∼37[MA∕(m∙T)] on NSTX. The behavior of ELMs is observed to depend on plasma shape. A description of the ELM regimes attained as shape is varied will be presented. Increased shaping is predicted to increase the bootstrap fraction at fixed Ip. The achievement of strong shaping ...


Fusion Engineering and Design | 2001

Engineering design of the National Spherical Torus Experiment

C. Neumeyer; P. Heitzenroeder; J Spitzer; J. Chrzanowski; A. Brooks; J. Bialek; H.-M. Fan; G. Barnes; M. Viola; B. Nelson; P. Goranson; R Wilson; E. Fredd; L. Dudek; R. Parsells; M. Kalish; W. Blanchard; R. Kaita; H.W. Kugel; B. McCormack; S. Ramakrishnan; R.E. Hatcher; G. Oliaro; E. Perry; T Egebo; A. von Halle; M. D. Williams; M. Ono

NSTX is a proof-of-principle experiment aimed at exploring the physics of the ‘spherical torus’ (ST) configuration, which is predicted to exhibit more efficient magnetic confinement than conventional large aspect ratio tokamaks, among other advantages. The low aspect ratio (R:a, typically 1.2‐2 in ST designs compared to 4‐5 in conventional tokamaks) decreases the available cross sectional area through the center of the torus for toroidal and poloidal field coil conductors, vacuum vessel wall, plasma facing components, etc., thus increasing the need to deploy all components within the so-called ‘center stack’ in the most efficient manner possible. Several unique design features have been developed for the NSTX center stack, and careful engineering of this region of the machine, utilizing materials up to their engineering allowables, has been key to meeting the desired objectives. The design and construction of the machine has been accomplished in a rapid and cost effective manner thanks to the availability of extensive facilities, a strong experience base from the TFTR era, and good cooperation between institutions.


ieee npss symposium on fusion engineering | 1999

NSTX electrical power systems

S. Ramakrishnan; C. Neumeyer; E. Baker; Ron Hatcher; A. Ilic; R. Marsala; D. O'Neill; A. von Halle

The National Spherical Torus Experiment (NSTX) has been designed and installed in the existing facilities at Princeton Plasma Physics Laboratory (PPPL). Most of the hardware, plant facilities, auxiliary sub-systems, and power systems originally used for the Tokamak Fusion Test Reactor (TFTR) have been used with suitable modifications to reflect NSTX needs. The design of the NSTX electrical power system was tailored to suit the available infrastructure and electrical equipment on site. Components were analyzed to verify their suitability for use in NSTX.


Plasma Physics and Controlled Fusion | 1994

Deuterium and tritium experiments on TFTR

J. D. Strachan; H. Adler; Cris W. Barnes; S.H. Batha; M.G. Bell; R. E. Bell; M. Bitter; N. Bretz; R.V. Budny; C.E. Bush; M. Caorlin; Z. Chang; D.S. Darrow; H.H. Duong; R Durst; P.C. Efthimion; R.K. Fisher; R.J. Fonck; E. D. Fredrickson; B. Grek; L.R. Grisham; G. W. Hammett; R J Hawryiuk; W. W. Heidbrink; H.W. Herrmann; K. W. Hill; J. Hosea; H. Hsuan; A. Janos; D.L. Jassby

Three campaigns, prior to July 1994, attempted to increase the fusion power in DT plasmas on the Tokamak Fusion Test Reactor (TFTR). The first campaign was dedicated to obtaining >5 MW of fusion power while avoiding MHD events similar to the JET X-event. The second was aimed at producing maximum fusion power irrespective of proximity to MHD limits, and achieved 9 MW limited by a disruption. The third campaign increased the energy confinement time using lithium pellet conditioning while raising the ratio of alpha heating to beam heating.


Review of Scientific Instruments | 1989

TFTR neutral beam injected power measurement

J. H. Kamperschroer; L. R. Grisham; L. Dudek; G. M. Gammel; G. A. Johnson; H.W. Kugel; L. J. Lagin; T. E. O’Connor; P. A. Shah; P. Sichta; T. Stevenson; A. von Halle; M. D. Williams; R. Bastasz

Energy flow within TFTR neutral beamlines is measured with a waterflow calorimetry system capable of simultaneously measuring the energy deposited within four heating beamlines (three ion sources each), or of measuring the energy deposited in a separate neutral beam test stand. Of the energy extracted from the ion source on the well‐instrumented test stand, 99.5±3.5% can be accounted for. When the ion deflection magnet is energized, however, 6.5% of the extracted energy is lost. This loss is attributed to a spray of devious particles onto unmonitored surfaces. A 30% discrepancy is also observed between energy measurements on the internal beamline calorimeter and energy measurements on a calorimeter located in the test stand target chamber. Particle reflection from the flat plate calorimeter in the target chamber, which the incident beam strikes at a near‐grazing angle of 12°, is the primary loss of this energy. A slight improvement in energy accountability is observed as the beam pulse length is increased...


international symposium on fusion engineering | 1995

The TFTR 40 MW neutral beam injection system and DT operations

T. Stevenson; T. O'Connor; V. Garzotto; L.R. Grisham; J.H. Kamperschroer; B.E. McCormack; R. Newman; M.E. Oldaker; S. Ramakrishnan; A. von Halle; K.E. Wright

Since December 1993, TFTR has performed DT experiments using tritium fuel provided mainly by neutral beam injection. Significant alpha particle populations and reactor-like conditions have been achieved at the plasma core, and fusion output power has risen to a record 10.7 MW using a record 40 MW NB heating. Tritium neutral beams have injected into over 480 DT plasmas and greater than 500 kCi have been processed through the neutral beam gas, cryo, and vacuum systems. Beam tritium injections, as well as tritium feedstock delivery and disposal, have now become part of routine operations. Shot reliability with tritium is about 90% and is comparable to deuterium shot reliability. This paper describes the neutral beam DT experience including the preparations, modifications, and operating techniques that led to this high level of success, as well as the critical differences in beam operations encountered during DT operations. Also, the neutral beam maintenance and repair history during DT operations, the corrective actions taken, and procedures developed for handling tritium contaminated components are discussed in the context of supporting a continuous DT program.


Journal of Vacuum Science and Technology | 1989

Gas utilization in the Tokamak Fusion Test Reactor neutral beam injectors

J.H. Kamperschroer; G. M. Gammel; H.W. Kugel; L.R. Grisham; T. Stevenson; A. von Halle; M. Williams; T. T. C. Jones

Measurements of gas utilization were performed using hydrogen and deuterium beams in the Tokamak Fusion Test Reactor (TFTR) neutral beam test beamline to study the feasibility of operating tritium beams with existing ion sources under conditions of minimal tritium consumption. (i) It was found that the fraction of gas molecules introduced into the TFTR long‐pulse ion sources that are converted to extracted ions (i.e., the ion source gas efficiency) was higher than with previous short‐pulse sources. Gas efficiencies were studied over the range 33%–55%, and its effect on neutralization of the extracted ions was studied. At the high end of the gas efficiency range, the neutral fraction of the beam fell below that predicted from room‐temperature molecular gas flow (similar to observations at the Joint European Torus). (ii) Beam isotope change studies were performed. No extracted hydrogen ions were observed in the first deuterium beam following a working gas change from H2 to D2. There was no arc conditioning ...

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T. Stevenson

Princeton Plasma Physics Laboratory

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L. Dudek

Princeton University

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G. Rossi

Princeton University

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L. R. Grisham

Princeton Plasma Physics Laboratory

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