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Featured researches published by H.W. Kugel.


Nuclear Fusion | 2000

Exploration of Spherical Torus Physics in the NSTX Device

M. Ono; S.M. Kaye; Yueng Kay Martin Peng; G. Barnes; W. Blanchard; Mark Dwain Carter; J. Chrzanowski; L. Dudek; R. Ewig; D.A. Gates; Ron Hatcher; Thomas R. Jarboe; S.C. Jardin; D. Johnson; R. Kaita; M. Kalish; C. Kessel; H.W. Kugel; R. Maingi; R. Majeski; J. Manickam; B. McCormack; J. Menard; D. Mueller; B.A. Nelson; B. E. Nelson; C. Neumeyer; G. Oliaro; F. Paoletti; R. Parsells

The National Spherical Torus Experiment (NSTX) is being built at the Princeton Plasma Physics Laboratory to test the fusion physics principles for the Spherical Torus (ST) concept at the MA level. The NSTX nominal plasma parameters are R {sub 0} = 85 cm, a = 67 cm, R/a greater than or equal to 1.26, B {sub T} = 3 kG, I {sub p} = 1 MA, q {sub 95} = 14, elongation {kappa} less than or equal to 2.2, triangularity {delta} less than or equal to 0.5, and plasma pulse length of up to 5 sec. The plasma heating/current drive (CD) tools are High Harmonic Fast Wave (HHFW) (6 MW, 5 sec), Neutral Beam Injection (NBI) (5 MW, 80 keV, 5 sec), and Coaxial Helicity Injection (CHI). Theoretical calculations predict that NSTX should provide exciting possibilities for exploring a number of important new physics regimes including very high plasma beta, naturally high plasma elongation, high bootstrap current fraction, absolute magnetic well, and high pressure driven sheared flow. In addition, the NSTX program plans to explore fully noninductive plasma start-up, as well as a dispersive scrape-off layer for heat and particle flux handling.


Nuclear Fusion | 2001

Equilibrium properties of spherical torus plasmas in NSTX

Steven Anthony Sabbagh; S.M. Kaye; J. Menard; F. Paoletti; M.G. Bell; R.E. Bell; J. Bialek; M. Bitter; E.D. Fredrickson; D.A. Gates; A.H. Glasser; H.W. Kugel; L. L. Lao; Benoit P. Leblanc; R. Maingi; Ricardo Jose Maqueda; E. Mazzucato; D. Mueller; M. Ono; S.F. Paul; M. J. Peng; C.H. Skinner; D. Stutman; G. A. Wurden; W. Zhu

Research in NSTX has been conducted to establish spherical torus plasmas to be used for high ?, auxiliary heated experiments. This device has a major radius R0 = 0.86?m and a midplane halfwidth of 0.7?m. It has been operated with toroidal magnetic field B0 ? 0.3?T and Ip ? 1.0?MA. The evolution of the plasma equilibrium is analysed between discharges with an automated version of the EFIT code. Limiter, double null and lower single null diverted configurations have been sustained for several energy confinement times. The plasma stored energy reached 92?kJ (?t = 17.8%) with neutral beam heating. A plasma elongation in the range 1.6 ? ? ? 2.0 and a triangularity in the range 0.25 ? ? ? 0.45 have been sustained, with values of ? = 2.6 and ? = 0.6 being reached transiently. The reconstructed magnetic signals are fitted to the corresponding measured values with low errors. Aspects of the plasma boundary, pressure and safety factor profiles are supported by measurements from non-magnetic diagnostics. Plasma densities have reached 0.8 and 1.2 times the Greenwald limit in deuterium and helium plasmas, respectively, with no clear limit encountered. Instabilities including sawteeth and reconnection events, characterized by Mirnov oscillations, and a perturbation of the Ip, ? and li evolutions, have been observed. A low q limit was observed and is imposed by a low toroidal mode number kink instability.


Plasma Physics and Controlled Fusion | 2009

Plasma response to lithium-coated plasma-facing components in the National Spherical Torus Experiment

M.G. Bell; H.W. Kugel; R. Kaita; Leonid E. Zakharov; H. Schneider; Benoit P. Leblanc; D.K. Mansfield; R.E. Bell; R. Maingi; S. Ding; S.M. Kaye; S. Paul; S.P. Gerhardt; John M. Canik; J. C. Hosea; G. Taylor

Experiments in the National Spherical Torus Experiment (NSTX) have shown beneficial effects on the performance of divertor plasmas as a result of applying lithium coatings on the graphite and carbon-fiber-composite plasma-facing components. These coatings have mostly been applied by a pair of lithium evaporators mounted at the top of the vacuum vessel which inject collimated streams of lithium vapor toward the lower divertor. In neutral beam injection (NBI)-heated deuterium H-mode plasmas run immediately after the application of lithium, performance modifications included decreases in the plasma density, particularly in the edge, and inductive flux consumption, and increases in the electron and ion temperatures and the energy confinement time. Reductions in the number and amplitude of edge-localized modes (ELMs) were observed, including complete ELM suppression for periods of up to 1.2 s, apparently as a result of altering the stability of the edge. However, in the plasmas where ELMs were suppressed, there was a significant secular increase in the effective ion charge Zeff and the radiated power as a result of increases in the carbon and medium-Z metallic impurities, although not of lithium itself which remained at a very low level in the plasma core, <0.1%. The impurity buildup could be inhibited by repetitively triggering ELMs with the application of brief pulses of an n = 3 radial field perturbation. The reduction in the edge density by lithium also inhibited parasitic losses through the scrape-off-layer of ICRF power coupled to the plasma, enabling the waves to heat electrons in the core of H-mode plasmas produced by NBI. Lithium has also been introduced by injecting a stream of chemically stabilized, fine lithium powder directly into the scrape-off-layer of NBI-heated plasmas. The lithium was ionized in the SOL and appeared to flow along the magnetic field to the divertor plates. This method of coating produced similar effects to the evaporated lithium but at lower amounts.


Nuclear Fusion | 2001

Observations concerning the injection of a lithium aerosol into the edge of TFTR discharges

D.K. Mansfield; D. Johnson; B. Grek; H.W. Kugel; M.G. Bell; R.E. Bell; R.V. Budny; C.E. Bush; E.D. Fredrickson; K. W. Hill; D. Jassby; Ricardo Jose Maqueda; H. Park; A.T. Ramsey; E. J. Synakowski; G. Taylor; G. A. Wurden

A new method of actively modifying the plasma-wall interaction was tested on the Tokamak Fusion Test Reactor. A laser was used to introduce a directed lithium aerosol into the discharge scrape-off layer. The lithium introduced in this fashion ablated and migrated preferentially to the limiter contact points. This allowed the plasma-wall interaction to be influenced in situ and in real time by external means. Significant improvement in energy confinement and fusion neutron production rate as well as a reduction in the plasma Zeff have been documented in a neutral beam heated plasma. The introduction of a metallic aerosol into the plasma edge increased the internal inductance of the plasma column and also resulted in prompt heating of core electrons in ohmic plasmas. Preliminary evidence also suggests that the introduction of an aerosol leads to both edge poloidal velocity shear and edge electric field shear.


Review of Scientific Instruments | 1990

Magnetic field pitch angle diagnostic using the motional Stark effect (invited)

F. M. Levinton; G. M. Gammel; R. Kaita; H.W. Kugel; D. W. Roberts

The Stark effect has been employed in a novel technique for obtaining the pitch angle profile and q(r) using polarimetry measurements of the Doppler shifted Hα emission from a hydrogen diagnostic neutral beam. As a neutral beam propagates through a plasma, collisions of the beam particles with the background ions and electrons will excite beam atoms, leading to emission of radiation. The motional Stark effect, which arises from the electric field induced in the atom’s rest frame due to the beam motion across the magnetic field (E=Vbeam×B), causes a wavelength splitting of several angstroms and polarization of the emitted radiation. The Δm=±1 transitions, or σ components, from the beam fluorescence are linearly polarized parallel to the direction of the local magnetic field when viewed transverse to the fields. Since the hydrogen beam provides good spatial localization and penetration, the pitch angle can be obtained anywhere in the plasma. A photoelastic modulator (PEM) is used to modulate the linearly po...


Review of Scientific Instruments | 2001

Edge turbulence measurements in NSTX by gas puff imaging

Ricardo Jose Maqueda; G. A. Wurden; S. J. Zweben; L. Roquemore; H.W. Kugel; D. Johnson; S.M. Kaye; S.A. Sabbagh; R. Maingi

Turbulent filaments in visible light emission corresponding mainly to density fluctuations at the edge have been observed in large aspect ratio tokamaks: TFTR, ASDEX, Alcator C-Mod, and DIII-D. This article reports on similar turbulent structures observed in the National Spherical Torus Experiment (NSTX) using a fast-framing, intensified, digital visible camera. These filaments were previously detected mainly in high recycling regions, such as at limiters or antennas, where the line emission from neutral atoms was modulated by the fluctuations in local plasma density. However, by introducing controlled edge gas puffs, i.e., gas puff imaging, we have increased the brightness and contrast in the fluctuation images and allowed the turbulent structure to be measured independently of the recycling. A set discrete fiber-optically coupled sight-lines also measured the frequency spectra of these light fluctuations with a 200 kHz bandwidth. Initial results in NSTX show that the turbulent filaments are well aligned...


Fusion Technology | 1999

Physics design of the national spherical torus experiment

S.M. Kaye; M. Ono; Yueng-Kay Martin Peng; D. B. Batchelor; Mark Dwain Carter; Wonho Choe; Robert J. Goldston; Yong-Seok Hwang; E. Fred Jaeger; Thomas R. Jarboe; Stephen C. Jardin; D.W. Johnson; R. Kaita; Charles Kessel; H.W. Kugel; R. Maingi; R. Majeski; Janhardan Manickam; J. Menard; David Mikkelsen; David J. Orvis; Brian A. Nelson; F. Paoletti; N. Pomphrey; Gregory Rewoldt; Steven Anthony Sabbagh; Dennis J Strickler; E. J. Synakowski; J. R. Wilson

The mission of the National Spherical Torus Experiment (NSTX) is to prove the principles of spherical torus physics by producing high-beta toroidal plasmas that are non-inductively sustained, and whose current profiles are in steady-state. NSTX will be one of the first ultra low a[P(input) up to 11 MW] in order to produce high-beta toroidal (25 to 40%), low collisionality, high bootstrap fraction (less than or equal to 70%) discharges. Both radio-frequency (RF) and neutral-beam (NB) heating and current drive will be employed. Built into NSTX is sufficient configurational flexibility to study a range of operating space and the resulting dependences of the confinement, micro- and MHD stability, and particle and power handling properties. NSTX research will be carried out by a nationally based science team.


Plasma Physics and Controlled Fusion | 2001

Initial results from coaxial helicity injection experiments in NSTX

R. Raman; Thomas R. Jarboe; D. Mueller; M.J. Schaffer; Ricardo Jose Maqueda; B.A. Nelson; S.A. Sabbagh; M.G. Bell; R. Ewig; E.D. Fredrickson; D.A. Gates; J. Hosea; Hantao Ji; R. Kaita; S.M. Kaye; H.W. Kugel; R. Maingi; J. Menard; M. Ono; D. Orvis; F. Paoletti; S. Paul; M. J. Peng; C.H. Skinner; J. B. Wilgen; S. J. Zweben

Coaxial helicity injection has been investigated on the National Spherical Torus Experiment (NSTX). Initial experiments produced 130 kA of toroidal current without the use of the central solenoid. The corresponding injector current was 20 kA. Discharges with pulse lengths up to 130 ms have been produced.


Physics of fluids. B, Plasma physics | 1990

Control of plasma shape and performance of the PBX‐M tokamak experiment in high‐βt /high‐βp regimes

R.E. Bell; N. Asakura; S. Bernabei; M. S. Chance; P.‐A. Duperrex; R. J. Fonck; G. M. Gammel; G. J. Greene; R. Hatcher; A. Holland; Stephen C. Jardin; T.‐W. Jiang; R. Kaita; S.M. Kaye; C. E. Kessel; H.W. Kugel; Benoit P. Leblanc; F. M. Levinton; M. Okabayashi; M. Ono; S. Paul; E. T. Powell; Y. Qin; D. W. Roberts; N. R. Sauthoff; S. Sesnic; H. Takahashi

The highly indented plasmas of the PBX‐M tokamak experiment [Plasma Physics and Controlled Nuclear Fusion Research (IAEA, Vienna, 1989), Vol. 1, p. 97] have reached plasma regimes of both high volume‐averaged beta (βt), and high‐beta poloidal (βp), and show evidence of the suppression of external surface modes by the passive stabilizing system. Values of βt up to 4.0 I/aB (% MA/m T) with Ti(0)≊4 keV have been obtained. A magnetohydrodynamic analysis of plasmas with βp=2.0 indicates that these plasmas are near the threshold of the second stability regime. A value of βt of 6.8% has been reached with Ti(0)>5 keV and an indentation of 28%. Control of plasma shape is accomplished with a feedback system that uses a moment expansion about a single equilibrium and is augmented by time‐dependent waveforms to redefine plasma shape. Diagnostics to measure the safety factor q have been developed and used to make accurate measurements of q(r) and to verify changes made in q(0).


Nuclear Fusion | 2010

ELM destabilization by externally applied non-axisymmetric magnetic perturbations in NSTX

John M. Canik; R. Maingi; T.E. Evans; R.E. Bell; S.P. Gerhardt; H.W. Kugel; Benoit P. Leblanc; J. Manickam; J. Menard; T.H. Osborne; Jin Myung Park; S. Paul; P.B. Snyder; S.A. Sabbagh; E.A. Unterberg

We report on a recent set of experiments performed in NSTX to explore the effects of non-axisymmetric magnetic perturbations on the stability of edge-localized modes (ELMs). The application of these 3D fields in NSTX was found to have a strong effect on ELM stability, including the destabilization of ELMs in H-modes otherwise free of large ELMs. Exploiting the effect of the perturbations, ELMs have been controllably introduced into lithium-enhanced ELM-free H-modes, causing a reduction in impurity accumulation while maintaining high confinement. Although these experiments show the principle of the combined use of lithium coatings and 3D fields, further optimization is required in order to reduce the size of the induced ELMs.

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R. Kaita

Princeton Plasma Physics Laboratory

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R. Maingi

Oak Ridge National Laboratory

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V. Soukhanovskii

Lawrence Livermore National Laboratory

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M.G. Bell

Princeton Plasma Physics Laboratory

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J. Menard

Princeton Plasma Physics Laboratory

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S.M. Kaye

Princeton Plasma Physics Laboratory

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Benoit P. Leblanc

Princeton Plasma Physics Laboratory

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D. Mueller

Princeton Plasma Physics Laboratory

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S. Paul

Princeton Plasma Physics Laboratory

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