Ronald Bravenec
University of Texas at Austin
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Ronald Bravenec.
Nuclear Fusion | 1989
S.C. McCool; A. J. Wootton; A. Y. Aydemir; Roger D. Bengtson; J.A. Boedo; Ronald Bravenec; D. L. Brower; J.S. DeGrassie; T.E. Evans; S.P. Fan; J.C. Forster; M.S. Foster; K. W. Gentle; Y.X. He; R.L. Hickock; G.L. Jackson; S.K. Kim; M. Kotschenreuther; N.C. Luhmann; William H. Miner; N. Ohyabu; D.M. Patterson; W. A. Peebles; P.E. Phillips; T.L. Rhodes; B. Richards; Ch. P. Ritz; David W. Ross; William L. Rowan; P. M. Schoch
Externally applied magnetic fields are used on the Texas Experimental Tokamak (TEXT) to study the possibility of controlling the particle, impurity and heat fluxes at the plasma edge. Fields with toroidal mode number n = 2 or 3 and multiple poloidal mode numbers m (dominantly m = 7) are used, with a poloidally and toroidally averaged ratio of radial to toroidal field components 〈|br/Bo〉 ≅0. 1%. Calculations show that it is possible to produce mixed islands and stochastic regions at the plasma edge (r/a ≥ 0.8) without affecting the interior. The expected magnetic field structure is described and experimental evidence of the existence of this structure is presented. The edge electron temperature decreases with increasing 〈|br/Bo〉, while interior values are not significantly affected. The implied increase in edge electron thermal diffusivity is compared with theoretical expectations and is shown to agree with applicable theories to within a factor of three.
Nuclear Fusion | 2005
M. Greenwald; D. Andelin; N. Basse; S. Bernabei; P.T. Bonoli; B. Böse; C. Boswell; Ronald Bravenec; B. A. Carreras; I. Cziegler; E. Edlund; D. Ernst; C. Fasoli; M. Ferrara; C. Fiore; R. Granetz; O. Grulke; T. C. Hender; J. Hosea; D.H. Howell; A. Hubbard; J.W. Hughes; Ian H. Hutchinson; A. Ince-Cushman; James H. Irby; B. LaBombard; R. J. LaHaye; L. Lin; Y. Lin; B. Lipschultz
Research on the Alcator C-Mod tokamak has emphasized RF heating, self-generated flows, momentum transport, scrape-off layer (SOL) turbulence and transport and the physics of transport barrier transitions, stability and control. The machine operates with P-RF up to 6 MW corresponding to power densities on the antenna of 10 MW m(-2). Analysis of rotation profile evolution, produced in the absence of external drive, allows transport of angular momentum in the plasma core to be computed and compared between various operating regimes. Momentum is clearly seen diffusing and convecting from the plasma edge on time scales similar to the energy confinement time and much faster than neo-classical transport. SOL turbulence and transport have been studied with fast scanning electrostatic probes situated at several poloidal locations and with gas puff imaging. Strong poloidal asymmetries are found in profiles and fluctuations, confirming the essential ballooning character of the turbulence and transport. Plasma topology has a dominant effect on the magnitude and direction of both core rotation and SOL flows. The correlation of self-generated plasma flows and topology has led to a novel explanation for the dependence of the H-mode power threshold on the del B drift direction. Research into internal transport barriers has focused on control of the barrier strength and location. The foot of the barrier could be moved to larger minor radius by lowering q or B-T. The barriers, which are produced in C-Mod by off-axis RF heating, can be weakened by the application of on-axis power. Gyro-kinetic simulations suggest that the control mechanism is due to the temperature dependence of trapped electron modes which are destabilized by the large density gradients. A set of non-axisymmetric coils was installed allowing intrinsic error fields to be measured and compensated. These also enabled the determination of the mode locking threshold and, by comparison with data from other machines, provided the first direct measurement of size scaling for the threshold. The installation of a new inboard limiter resulted in the reduction of halo currents following disruptions. This effect can be understood in terms of the change in plasma contact with the altered geometry during vertical displacement of the plasma column. Unstable Alfven eigenmodes (AE) were observed in low-density, high-power ICRF heated plasmas. The damping rate of stable AEs was investigated with a pair of active MHD antennae.
Nuclear Fusion | 1989
D. L. Brower; M. H. Redi; W. M. Tang; Ronald Bravenec; R.D. Durst; S.P. Fan; Y.X. He; S.K. Kim; N.C. Luhmann; S.C. McCool; A.G. Meigs; M. Nagatsu; A. Ouroua; W. A. Peebles; P.E. Phillips; T.L. Rhodes; B. Richards; Ch. P. Ritz; William L. Rowan; A. J. Wootton
For high density Ohmic discharges in the TEXT tokamak, a distinct ion mode (i.e. density fluctuations propagating in the ion diamagnetic drift direction) is observed in the microturbulence spectra. The magnitude and spectral characteristics of the mode are identified. A microinstability based transport model is used for the purpose of interpreting anomalous confinement properties. Onset of the ion feature occurs at plasma densities where a clear saturation is evident in the global energy confinement time τE. When the ion feature in the fluctuation spectra is strongest, agreement between predictions from the transport model and experimentally measured values of the global energy confinement time is realized if anomalous ion effects due to the ion pressure gradient driven (ηi) instability are included. By injecting pellets, a high density plasma is created in which the density profile is sharply peaked. Under these conditions the ion feature in the fluctuation spectra is suppressed. A possible connection between this experimentally observed ion mode and the theoretically predicted properties of the ηi instability is explored.
Nuclear Fusion | 2007
Stacey D. Scott; A. Bader; M. Bakhtiari; N. Basse; W. Beck; T. M. Biewer; S. Bernabei; P.T. Bonoli; B. Böse; Ronald Bravenec; I.O. Bespamyatnov; R. Childs; I. Cziegler; R.P. Doerner; E. Edlund; D. Ernst; A. Fasoli; M. Ferrara; C. Fiore; T. Fredian; A. Graf; T. Graves; R. Granetz; N.L. Greenough; M. Greenwald; M. Grimes; O. Grulke; D. Gwinn; R. W. Harvey; S. Harrison
Alcator C-MOD has compared plasma performance with plasma-facing components (PFCs) coated with boron to all-metal PFCs to assess projections of energy confinement from current experiments to next-generation burning tokamak plasmas. Low-Z coatings reduce metallic impurity influx and diminish radiative losses leading to higher H-mode pedestal pressure that improves global energy confinement through profile stiffness. RF sheath rectification along flux tubes that intersect the RF antenna is found to be a major cause of localized boron erosion and impurity generation. Initial lower hybrid current drive (LHCD) experiments (PLH < 900?kW) in preparation for future advanced-tokamak studies have demonstrated fully non-inductive current drive at Ip ~ 1.0?MA with good efficiency, Idrive = 0.4 PLH/neoR (MA, MW, 1020?m?3,m). The potential to mitigate disruptions in ITER through massive gas-jet impurity puffing has been extended to significantly higher plasma pressures and shorter disruption times. The fraction of total plasma energy radiated increases with the Z of the impurity gas, reaching 90% for krypton. A positive major-radius scaling of the error field threshold for locked modes (Bth/B ? R0.68?0.19) is inferred from its measured variation with BT that implies a favourable threshold value for ITER. A phase contrast imaging diagnostic has been used to study the structure of Alfv?n cascades and turbulent density fluctuations in plasmas with an internal transport barrier. Understanding the mechanisms responsible for regulating the H-mode pedestal height is also crucial for projecting performance in ITER. Modelling of H-mode edge fuelling indicates high self-screening to neutrals in the pedestal and scrape-off layer (SOL), and reproduces experimental density pedestal response to changes in neutral source, including a weak variation of pedestal height and constant width. Pressure gradients in the near SOL of Ohmic L-mode plasmas are observed to scale consistently as , and show a significant dependence on X-point topology. Fast camera images of intermittent turbulent structures at the plasma edge show they travel coherently through the SOL with a broad radial velocity distribution having a peak at about 1% of the ion sound speed, in qualitative agreement with theoretical models. Fast D? diagnostics during gas puff imaging show a complex behaviour of discrete ELMs, starting with an n ? 10 precursor oscillation followed by a rapid primary ejection as the pedestal crashes and then multiple, slower secondary ejections.
Nuclear Fusion | 1985
N. Ohyabu; J.S. deGrassie; N. Brooks; T. Taylor; H. Ikezi; K. W. Gentle; Roger D. Bengtson; Ronald Bravenec; W L Hodge; K. Nelin; P.E. Phillips; B. Richards; Ch. P. Ritz; William L. Rowan; Y.X. Wan; C.C. Klepper; J.L. Porter; J.A. Snipes
The Ergodic Magnetic Layer Experiment on ohmically heated Text demonstrates that a small resonant helical field (m/n = 7/2 or 7/3) with fractional amplitude r/BT of about 10−3 creates a stable ergodic magnetic layer and substantially modifies the boundary heat flow. Field line tracings accurately map the observed perturbed limiter heat load patterns. The level of the intrinsic impurities is reduced, consistent with a lower edge electron temperature, as measured by the electron cyclotron emission detector.
Physics of Plasmas | 2011
Ronald Bravenec; J. Candy; M. Barnes; C. Holland
Verification of nonlinear microstability codes is a necessary step before comparisons or predictions of turbulent transport in toroidal devices can be justified. By verification we mean demonstrating that a code correctly solves the mathematical model upon which it is based. Some degree of verification can be accomplished indirectly from analytical instability threshold conditions, nonlinear saturation estimates, etc., for relatively simple plasmas. However, verification for experimentally relevant plasma conditions and physics is beyond the realm of analytical treatment and must rely on code-to-code comparisons, i.e., benchmarking. The premise is that the codes are verified for a given problem or set of parameters if they all agree within a specified tolerance. True verification requires comparisons for a number of plasma conditions, e.g., different devices, discharges, times, and radii. Running the codes and keeping track of linear and nonlinear inputs and results for all conditions could be prohibitive...
Physics of Plasmas | 2002
David W. Ross; Ronald Bravenec; William Dorland; Michael Beer; G. W. Hammett; G.R. McKee; R. J. Fonck; M. Murakami; Keith H. Burrell; G.L. Jackson; G. M. Staebler
The direct quantitative correspondence between theoretical predictions and the measured plasma fluctuations and transport is tested by performing nonlinear gyro-Landau-fluid simulations with the GRYFFIN (or ITG) code [W. Dorland and G. W. Hammett, Phys. Fluids B 5, 812 (1993); M. A. Beer and G. W. Hammett, Phys. Plasmas 3, 4046 (1996)]. In an L-mode reference discharge in the DIII-D tokamak [J. L. Luxon and L. G. Davis, Fusion Technol. 8, 441 (1985)], which has relatively large fluctuations and transport, the turbulence is dominated by ion temperature gradient (ITG) modes. Trapped electron modes and impurity drift waves also play a role. Density fluctuations are measured by beam emission spectroscopy [R. J. Fonck, P. A. Duperrex, and S. F. Paul, Rev. Sci. Instrum. 61, 3487 (1990)]. Experimental fluxes and corresponding diffusivities are analyzed by the TRANSP code [R. J. Hawryluk, in Physics of Plasmas Close to Thermonuclear Conditions, edited by B. Coppi, G. G. Leotta, D. Pfirsch, R. Pozzoli, and E. Sind...
Nuclear Fusion | 2001
Ian H. Hutchinson; R. L. Boivin; P.T. Bonoli; C. Boswell; Ronald Bravenec; N.L. Bretz; R. Chatterjee; T. Chung; E. Eisner; C. Fiore; S. Gangadhara; K. Gentle; Jennifer Ann Goetz; R. Granetz; M. Greenwald; J. Hosea; A. Hubbard; J.W. Hughes; Y. In; James H. Irby; B. LaBombard; Y. Lin; B. Lipschultz; Ricardo Jose Maqueda; E. Marmar; A. Mazurenko; D. Mikkelsen; D. A. Mossessian; R. Nachtrieb; R. Nazikian
Research on the Alcator C-Mod tokamak is focused on exploiting compact high density plasmas to understand core transport and heating, the physics of the H mode transport barrier, and the dynamics of the scrape-off layer and divertor. Rapid toroidal acceleration of the plasma core is observed during ohmic heated H modes and indicates a momentum pinch or similar transport mechanism. Core thermal transport observations support a critical gradient interpretation, but with gradients that disagree with present theoretical values. High resolution measurements of the H mode barrier have been obtained, including impurity and neutral densities, and the instability apparently responsible for the favourable `enhanced D alpha regime has been identified. Divertor bypass dynamic control experiments have directly addressed the important questions surrounding main chamber recycling and the effect of divertor closure on impurities and confinement. Future plans include quasi-steady-state advanced tokamak plasmas using lower hybrid current drive.
Nuclear Fusion | 2003
E.S. Marmar; B. Bai; R.L. Boivin; P.T. Bonoli; C. Boswell; Ronald Bravenec; B. A. Carreras; D. Ernst; C. Fiore; S. Gangadhara; K. Gentle; J.A. Goetz; R. Granetz; M. Greenwald; K. Hallatschek; J. Hastie; J. Hosea; A. Hubbard; J.W. Hughes; Ian H. Hutchinson; Y. In; James H. Irby; T. Jennings; D. Kopon; G.J. Kramer; B. LaBombard; W.D. Lee; Y. Lin; B. Lipschultz; J. Liptac
Research on the Alcator C-Mod tokamak [1] is focused on high particle- and power-density plasma regimes to understand particle and energy transport in the core, the dynamics of the H-mode pedestal, and scrape-off layer and divertor physics. The auxiliary heating is provided exclusively by RF waves, and both the physics and technology of RF heating and current drive are studied. The momentum which is manifested in strong toroidal rotation, in the absence of direct momentum input, has been shown to be transported in from the edge of the plasma following the L-H transition, with timescale comparable to that for energy transport. In discharges which develop internal transport barriers, the rotation slows first inside the barrier region, and then subsequently outside of the barrier foot. Heat pulse propagation studies using sawteeth indicate a very narrow region of strongly reduced energy transport, located near r/a = 0.5. Addition of on-axis ICRF heating arrests the buildup of density and impurities, leading to quasi-steady conditions. The quasi-coherent mode associated with enhanced D-Alpha (EDA) H-mode appears to be due to a resistive ballooning instability. As the pedestal pressure gradient and temperature are increased in EDA H-mode, small ELMs appear; detailed modelling indicates that these are due to intermediate n peeling-ballooning modes. Phase contrast imaging has been used to directly detect density fluctuations driven by ICRF waves in the core of the plasma, and mode conversion to an intermediate wavelength ion cyclotron wave has been observed for the first time. The bursty turbulent density fluctuations, observed to drive rapid cross-field particle transport in the edge plasma, appear to play a key role in the dynamics of the density limit. Preparations for quasi-steady-state advanced tokamak studies with lower hybrid current drive are well underway, and time dependent modelling indicates that regimes with high bootstrap fraction can be produced.
Nuclear Fusion | 1990
A. Ouroua; A. J. Wootton; Ronald Bravenec; Roger D. Bengtson; M. E. Austin; Jiayu Chen; R.F. Gandy; P.E. Phillips; B. Richards; Zemin Zhang
Profiles of the ion thermal diffusion coefficient χi have been determined experimentally for several TEXT plasma discharges. In the confinement region, the inferred values of χi are larger than the values predicted by neoclassical theory by a factor of two to six. No evidence of a reduction of thermal losses through the ion channel is found after injection of hydrogen pellets. The inferred electron thermal conductivities are larger than the ion thermal conductivities by an average factor of three. The anomaly in χi is compared with transport coefficients predicted by different models that describe the ηi instability.