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Dive into the research topics where D.P. Stotler is active.

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Featured researches published by D.P. Stotler.


Physics of Plasmas | 2003

Observations of the turbulence in the scrape-off-layer of Alcator C-Mod and comparisons with simulation

J. L. Terry; S.J. Zweben; K. Hallatschek; B. LaBombard; R. J. Maqueda; B. Bai; C. J. Boswell; M. Greenwald; D. Kopon; W. M. Nevins; C. S. Pitcher; B. N. Rogers; D.P. Stotler; X. Q. Xu

The intermittent turbulent transport in the scrape-off-layer (SOL) of Alcator C-Mod [I.H. Hutchinson, R. Boivin, P.T. Bonoli et al., Nucl. Fusion 41, 1391 (2001)] is studied experimentally by imaging with a very high density of spatial measurements. The two-dimensional structure and dynamics of emission from a localized gas puff are observed, and intermittent features (also sometimes called “filaments” or “blobs”) are typically seen. The characteristics of the spatial structure of the turbulence and their relationship to the time-averaged SOL profiles are discussed and compared with those measured on the National Spherical Torus Experiment [M. Ono, S. M. Kaye, Y.-K. M. Pong et al., Nucl. Fusion 40, 557 (2000)]. The experimental observations are compared also with three-dimensional nonlinear numerical simulations of edge turbulence. Radial profiles of the poloidal wave number spectra and the poloidal scale length from the simulations are in reasonable agreement with those obtained from the experimental ima...


Review of Scientific Instruments | 2003

Gas puff imaging of edge turbulence (invited)

Ricardo Jose Maqueda; G. A. Wurden; D.P. Stotler; S. J. Zweben; B. LaBombard; J. L. Terry; John L. Lowrance; V.J. Mastrocola; George F. Renda; D. A. D’Ippolito; J. R. Myra; N. Nishino

The gas puff imaging (GPI) diagnostic can be used to study the turbulence present at the edge of magnetically confined plasmas. In this diagnostic the instantaneous two-dimensional (2D) radial vs poloidal structure of the turbulence is measured using fast-gated cameras and discrete fast chords. By imaging a controlled neutral gas puff, of typically helium or deuterium, the brightness and contrast of the turbulent emission fluctuations are increased and the structure can be measured independently of natural gas recycling. In addition, recent advances in ultrafast framing cameras allow the turbulence to be followed in time. The gas puff itself does not perturb the edge turbulence and the neutral gas does not introduce fluctuations in the emission that could possibly arise from a nonsmooth (turbulent) neutral gas puff. Results from neutral transport and atomic physics simulations using the DEGAS 2 code are discussed showing that the observed line emission is sensitive to modulations in both the electron density and the electron temperature. The GPI diagnostic implementation in the National Spherical Torus Experiment (NSTX) and Alcator C-Mod tokamak is presented together with example results from these two experiments.


Physics of Plasmas | 2006

Blob birth and transport in the tokamak edge plasma: analysis of imaging data

J.R. Myra; D. A. D’Ippolito; D.P. Stotler; S.J. Zweben; Benoit P. Leblanc; J. Menard; R. Maqueda; J.A. Boedo

High-speed high-spatial-resolution data obtained by the gas puff imaging (GPI) diagnostic on the National Spherical Torus Experiment [M. Ono, M.G. Bell, R.E. Bell et al. Plasma Phys. Control. Fusion 45, A335 (2003).] is analyzed and interpreted in light of recent theoretical models for electrostatic edge turbulence and blob propagation. The experiment is described in terms of theoretical regimes that predict different dependencies for the radial velocity of blob convection. Using the GPI data, atomic physics analysis, and blob tracking on a restricted dataset, it is shown that the observed blob velocities in the scrape-off layer are bounded by a theory-based minimum velocity associated with the sheath-connected regime. A similar maximum velocity bound associated with the resistive-ballooning regime is also observed. Turning to the question of blob creation, it is shown that blobs are born with a density and temperature characteristic of the plasma conditions where underlying linear edge drift-curvature in...


Physics of Plasmas | 2006

Structure and motion of edge turbulence in the National Spherical Torus Experiment and Alcator C-Mod

Stewart J. Zweben; R. Maqueda; J. L. Terry; T. Munsat; J. Myra; D. A. D’Ippolito; D. A. Russell; J. A. Krommes; Benoit P. Leblanc; T. Stoltzfus-Dueck; D.P. Stotler; K. M. Williams; C.E. Bush; R. Maingi; O. Grulke; S.A. Sabbagh; A.E. White

In this paper we compare the structure and motion of edge turbulence observed in L-mode vs. H-mode plasmas in the National Spherical Torus Experiment (NSTX) [M. Ono, M. G. Bell, R. E. Bell et al., Plasma Phys. Controlled Fusion 45, A335 (2003)]. The radial and poloidal correlation lengths are not significantly different between the L-mode and the H-mode in the cases examined. The poloidal velocity fluctuations are lower and the radial profiles of the poloidal turbulence velocity are somewhat flatter in the H-mode compared with the L-mode plasmas. These results are compared with similar measurements Alcator C-Mod [E. Marmar, B. Bai, R. L. Boivin et al., Nucl. Fusion 43, 1610 (2003)], and with theoretical models.


Physics of Plasmas | 2010

Quiet periods in edge turbulence preceding the L-H transition in the National Spherical Torus Experiment

Stewart J. Zweben; R. J. Maqueda; Robert Hager; K. Hallatschek; S.M. Kaye; T. Munsat; Francesca M. Poli; A.L. Roquemore; Y. Sechrest; D.P. Stotler

This paper describes the first observations in the National Spherical Torus Experiment (NSTX) [S. M. Kaye et al., Phys. Plasmas 8, 1977 (2001)] of “quiet periods” in the edge turbulence preceding the low-to-high (L-H) mode transition, as diagnosed by the gas puff imaging (GPI) diagnostic near the outer midplane separatrix. During these quiet periods the GPI Dα light emission pattern was transiently similar to that seen during H-mode, i.e., with a relatively small fraction of the GPI light emission located outside the separatrix. These quiet periods had a frequency of ∼3 kHz for at least 30 ms before the L-H transition, and were correlated with changes in the direction of the local poloidal velocity. The GPI turbulence images were also analyzed to obtain an estimate for the dimensionless poloidal shearing S=(dVp/dr)(Lr/Lp)τ. The values of S were strongly modulated by the quiet periods but did not significantly vary during the ∼30 ms preceding the L-H transition. Since neither the quiet periods nor the shea...


Nuclear Fusion | 2009

Performance projections for the lithium tokamak experiment (LTX)

R. Majeski; L. Berzak; T. Gray; R. Kaita; Thomas Kozub; F. M. Levinton; D.P. Lundberg; J. Manickam; G. Pereverzev; K. Snieckus; V. Soukhanovskii; J. Spaleta; D.P. Stotler; T. Strickler; J. Timberlake; Jongsoo Yoo; Leonid E. Zakharov

Use of a large-area liquid lithium limiter in the CDX-U tokamak produced the largest relative increase (an enhancement factor of 5-10) in Ohmic tokamak confinement ever observed. The confinement results from CDX-U do not agree with existing scaling laws, and cannot easily be projected to the new lithium tokamak experiment (LTX). Numerical simulations of CDX-U low recycling discharges have now been performed with the ASTRA-ESC code with a special reference transport model suitable for a diffusion-based confinement regime, incorporating boundary conditions for nonrecycling walls, with fuelling via edge gas puffing. This model has been successful at reproducing the experimental values of the energy confinement (4-6 ms), loop voltage (<0.5 V), and density for a typical CDX-U lithium discharge. The same transport model has also been used to project the performance of the LTX, in Ohmic operation, or with modest neutral beam injection (NBI). NBI in LTX, with a low recycling wall of liquid lithium, is predicted to result in core electron and ion temperatures of 1-2 keV, and energy confinement times in excess of 50 ms. Finally, the unique design features of LTX are summarized.


Journal of Nuclear Materials | 2003

Neutral transport simulations of gas puff imaging experiments

D.P. Stotler; B. LaBombard; J. L. Terry; S.J. Zweben

Visible imaging of gas puffs has been used on the Alcator C-Mod tokamak to characterize edge plasma turbulence, yielding data that can be compared with plasma turbulence codes. Simulations of these experiments with the DEGAS 2 Monte Carlo neutral transport code have been carried out to explore the relationship between the plasma fluctuations and the observed light emission. By imposing two-dimensional modulations on the measured time-average plasma density and temperature profiles, we demonstrate that the spatial structure of the emission cloud reflects that of the underlying turbulence. However, the photon emission rate depends on the plasma density and temperature in a complicated way, and no simple scheme for inferring the plasma parameters directly from the light emission patterns is apparent. The simulations indicate that excited atoms generated by molecular dissociation are a significant source of photons, further complicating interpretation of the gas puff imaging results.


Physics of Plasmas | 2011

Reduced model simulations of the scrape-off-layer heat-flux width and comparison with experiment

J. R. Myra; D. A. Russell; D. A. D’Ippolito; J.-W. Ahn; R. Maingi; R. J. Maqueda; D. P. Lundberg; D.P. Stotler; S.J. Zweben; J.A. Boedo; M. V. Umansky; Nstx Team

Reduced model simulations of turbulence in the edge and scrape-off-layer (SOL) region of a spherical torus or tokamak plasma are employed to address the physics of the scrape-off-layer heat-flux width. The simulation model is an electrostatic two-dimensional fluid turbulence model, applied in the plane perpendicular to the magnetic field at the outboard midplane of the torus. The model contains curvature-driven-interchange modes, sheath losses, and both perpendicular turbulent diffusive and convective (blob) transport. These transport processes compete with classical parallel transport to set the SOL width. Midplane SOL profiles of density, temperature, and parallel heat flux are obtained from the simulation and compared with experimental results from the National Spherical Torus Experiment [S. M. Kaye et al., Phys. Plasmas 8, 1977 (2001)] to study the scaling of the heat-flux width with power and plasma current. It is concluded that midplane turbulence is the main contributor to the SOL heat-flux width f...


Physics of Plasmas | 2001

Initial physics results from the National Spherical Torus Experiment

S.M. Kaye; M.G. Bell; R. E. Bell; J. Bialek; T. Bigelow; M. Bitter; P.T. Bonoli; D. S. Darrow; Philip C. Efthimion; J.R. Ferron; E.D. Fredrickson; D.A. Gates; L. Grisham; J. Hosea; D.W. Johnson; R. Kaita; S. Kubota; H.W. Kugel; Benoit P. Leblanc; R. Maingi; J. Manickam; T. K. Mau; R. J. Maqueda; E. Mazzucato; J. Menard; D. Mueller; B.A. Nelson; N. Nishino; M. Ono; F. Paoletti

The mission of the National Spherical Torus Experiment (NSTX) is to extend the understanding of toroidal physics to low aspect ratio (R/a approximately equal to 1.25) in low collisionality regimes. NSTX is designed to operate with up to 6 MW of High Harmonic Fast Wave (HHFW) heating and current drive, 5 MW of Neutral Beam Injection (NBI) and Co-Axial Helicity Injection (CHI) for non-inductive startup. Initial experiments focused on establishing conditions that will allow NSTX to achieve its aims of simultaneous high-bt and high-bootstrap current fraction, and to develop methods for non-inductive operation, which will be necessary for Spherical Torus power plants. Ohmic discharges with plasma currents up to 1 MA and with a range of shapes and configurations were produced. Density limits in deuterium and helium reached 80% and 120% of the Greenwald limit respectively. Significant electron heating was observed with up to 2.3 MW of HHFW. Up to 270 kA of toroidal current for up to 200 msec was produced noninductively using CHI. Initial NBI experiments were carried out with up to two beam sources (3.2 MW). Plasmas with stored energies of up to 140 kJ and bt =21% were produced.


Physics of Plasmas | 2007

Study of statistical properties of edge turbulence in the National Spherical Torus Experiment with the gas puff imaging diagnostic

M. Agostini; S.J. Zweben; R. Cavazzana; P. Scarin; G. Serianni; R. Maqueda; D.P. Stotler

An investigation is presented of the edge turbulence in the National Spherical Torus Experiment [M. Ono, M. G. Bell, R. E. Bell et al., Plasma Phys. Control. Fusion, 45, A335 (2003)] based on the optical gas puff imaging (GPI) diagnostic. First of all, the edge fluctuations are characterized for the low confinement mode (L-mode) discharges as a function of the radius. The probability distribution function of the fluctuations is shown to be non-Gaussian for all the radial positions studied, but the deviation from the normal distribution is greater outside the separatrix; in this region the area occupied by the edge structures (“blobs”) is greater than inside the separatrix, and this is correlated with the decrease of the logarithmic radial derivative of the pressure gradient. Then the difference between the L-mode and the high confinement mode (H-mode) is studied. With the continuous wavelet transform technique the intense bursts in the GPI signal can be detected; their number decreases in the H-mode with ...

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R. Maingi

Princeton Plasma Physics Laboratory

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R. Kaita

Princeton University

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Benoit P. Leblanc

Princeton Plasma Physics Laboratory

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H.W. Kugel

Princeton Plasma Physics Laboratory

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S.J. Zweben

Princeton Plasma Physics Laboratory

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V. Soukhanovskii

Lawrence Livermore National Laboratory

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Ricardo Jose Maqueda

Los Alamos National Laboratory

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R. Maqueda

Princeton Plasma Physics Laboratory

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Stewart J. Zweben

Princeton Plasma Physics Laboratory

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