G. McCracken
Massachusetts Institute of Technology
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Featured researches published by G. McCracken.
Physics of Plasmas | 1994
Ian H. Hutchinson; R. L. Boivin; F. Bombarda; P.T. Bonoli; S. Fairfax; C. Fiore; Jennifer Ann Goetz; S. Golovato; R. Granetz; M. Greenwald; S. Horne; A. Hubbard; James H. Irby; B. LaBombard; B. Lipschultz; E. Marmar; G. McCracken; M. Porkolab; J. E. Rice; J. A. Snipes; Y. Takase; J. L. Terry; S.M. Wolfe; C. Christensen; D. Garnier; M. Graf; T. Hsu; T. Luke; M. May; A. Niemczewski
Early operation of the Alcator‐C‐MOD tokamak [I.H. Hutchinson, Proceedings of IEEE 13th Symposium on Fusion Engineering, Knoxville, TN, edited by M. Lubell, M. Nestor, and S. Vaughan (Institute of Electrical and Electronic Engineers, New York, 1990), Vol. 1, p. 13] is surveyed. Reliable operation, with plasma current up to 1 MA, has been obtained, despite the massive conducting superstructure and the associated error fields. However, vertical disruptions are not slowed by the long vessel time constant. With pellet fueling, peak densities up to 9×1020 m−3 have been attained and ‘‘snakes’’ are often seen. Initial characterization of divertor and scrape‐off layer is presented and indicates approximately Bohm diffusion. The edge plasma shows a wealth of marfe‐like phenomena, including a transition to detachment from the divertor plates with accompanying radiative divertor regions. Energy confinement generally appears to exceed the expectations of neo‐Alcator scaling. A transition to Ohmic H mode has been observed. Ion cyclotron heating experiments have demonstrated good power coupling, in agreement with theory.
Journal of Nuclear Materials | 1997
B. LaBombard; Jennifer Ann Goetz; Ian H. Hutchinson; D. Jablonski; J. Kesner; C. Kurz; B. Lipschultz; G. McCracken; A. Niemczewski; J. L. Terry; A. J. Allen; R. L. Boivin; F. Bombarda; P.T. Bonoli; C. Christensen; C. Fiore; D. Garnier; S. Golovato; R. Granetz; M. Greenwald; S. Horne; A. Hubbard; James H. Irby; D. Lo; D. Lumma; E. Marmar; M. May; A. Mazurenko; R. Nachtrieb; H. Ohkawa
Abstract Transport physics in the divertor and scrape-off layer of Alcator C-Mod is investigated for a wide range of plasma conditions. Parallel (∥) transport topics include: low recycling, high-recycling, and detached regimes, thermoelectric currents, asymmetric heat fluxes driven by thermoelectric currents, and reversed divertor flows. Perpendicular (⊥) transport topics include: expected and measured scalings of ⊥ gradients with local conditions, estimated χ⊥ profiles and scalings, divertor neutral retention effects, and L-mode/H-mode effects. Key results are: (i) classical ∥ transport is obeyed with ion-neutral momentum coupling effects, (ii) ⊥ heat transport is proportional to local gradients, (iii) χ⊥ αTe−0.6 n−0.6 L−0.7 in L-mode, insensitive to toroidal field, (iv) χ⊥ is dependent on divertor neutral retention, (v) H-mode transport barrier effects partially extend inside the SOL, (vi) inside/outside divertor asymmetries may be caused by a thermoelectric instability, and (vii) reversed ∥ flows depend on divertor asymmetries and their implicit ionization source imbalances.
Physics of Plasmas | 1995
B. LaBombard; Jennifer Ann Goetz; C. Kurz; D. Jablonski; B. Lipschultz; G. McCracken; A. Niemczewski; R. L. Boivin; F. Bombarda; C. Christensen; S. Fairfax; C. Fiore; D. Garnier; M. Graf; S. Golovato; R. Granetz; M. Greenwald; S. Horne; A. Hubbard; Ian H. Hutchinson; James H. Irby; J. Kesner; T. Luke; E. Marmar; M. May; P. O’Shea; M. Porkolab; J. Reardon; J. E. Rice; J. Schachter
Detailed measurements and transport analysis of divertor conditions in Alcator C‐Mod [Phys. Plasmas 1, 1511 (1994)] are presented for a range of line‐averaged densities, 0.7<ne<2.2×1020 m−3. Three parallel heat transport regimes are evident in the scrape‐off layer: sheath‐limited conduction, high‐recycling divertor, and detached divertor, which can coexist in the same discharge. Local cross‐field pressure gradients are found to scale simply with a local electron temperature. This scaling is consistent with classical electron parallel conduction being balanced by anomalous cross‐field transport (χ⊥∼0.2 m2 s−1) proportional to the local pressure gradient. A 60%–80% of divertor power is radiated in attached discharges, approaching 100% in detached discharges. Detachment occurs when the heat flux to the plate is low and the plasma pressure is high (Te∼5 eV). High neutral pressures in the divertor are nearly always present (1–20 mTorr), sufficient to remove parallel momentum via ion–neutral collisions.
Journal of Nuclear Materials | 1995
B. Lipschultz; Jennifer Ann Goetz; B. LaBombard; G. McCracken; J. L. Terry; M. Graf; R. Granetz; D. Jablonski; C. Kurz; A. Niemczewski; J. A. Snipes
The achievement of large volumetric power losses (dissipation) in the Alcator C-Mod divertor region is demonstrated in two operational modes: radiative divertor and detached divertor. During radiative divertor operation, the fraction of SOL power lost by radiation is P R /P SOL 0.8 with single null plasmas, n e < 2 × 10 20 m −3 and I p < 1 MA. THESE PLASMAS SOMETIMES HAVE VERY HIGH RECYCLING, WITH N e, div ≤ 6 x 10 20 m −3 . As the divertor radiation and density increase, the plasma eventually detaches abruptly from the divertor plates: I SAT drops at the target and the divertor radiation peak moves to the X-point region. Probe measurements at the divertor plate show that the transition occurs when T e 5 eV. The critical n e for detachment depends linearly on the input power. This abrupt divertor detachment is preceded by a comparatively long period (∼ 1-200 ms) where a partial detachment is observed to grow at the outer divertor plate
Physics of Plasmas | 1997
Y. Takase; R. L. Boivin; F. Bombarda; P.T. Bonoli; C. Christensen; C. Fiore; D. Garnier; Jennifer Ann Goetz; S. Golovato; R. Granetz; M. Greenwald; S. Horne; A. Hubbard; Ian H. Hutchinson; James H. Irby; B. LaBombard; B. Lipschultz; E. Marmar; M. May; A. Mazurenko; G. McCracken; P. O’Shea; M. Porkolab; James Christian Reardon; J. E. Rice; C. Rost; J. Schachter; J. A. Snipes; P. Stek; J. L. Terry
Enhanced confinement modes up to a toroidal field of BT=8 T have been studied with up to 3.5 MW of radiofrequency (rf) heating power in the ion cyclotron range of frequencies (ICRF) at 80 MHz. H-mode is observed when the edge temperature exceeds a threshold value. The high confinement mode (H-mode) with higher confinement enhancement factors (H) and longer duration became possible after boronization by reducing the radiated power from the main plasma. A quasi-steady state with high confinement (H=2.0), high normalized beta (βN=1.5), low radiated power fraction (Pradmain/Ploss=0.3), and low effective charge (Zeff=1.5) has been obtained in Enhanced Dα H-mode. This type of H-mode has enhanced levels of continuous Dα emission and very little or no edge localized mode (ELM) activity, and reduced core particle confinement time relative to ELM-free H-mode. The pellet enhanced performance (PEP) mode is obtained by combining core fueling with pellet injection and core heating. A highly peaked pressure profile with...
Journal of Nuclear Materials | 1999
William R. Wampler; B. LaBombard; B. Lipschultz; G. McCracken; D. Pappas; C. S. Pitcher
Erosion of molybdenum was measured on a set of 21 tiles after a run campaign of 1090 shots in the Alcator C-Mod tokamak. The net erosion of molybdenum was determined from changes in the depth of a thin chromium marker layer measured by Rutherford backscattering. Net Mo erosion was found to be approximately 150 nm near the outer divertor strikepoint and much less everywhere else. Gross erosion rates by sputtering were estimated using ion energies and fluxes obtained from Langmuir probe measurements of edge-plasma conditions. Predicted net erosion using calculated gross erosion with prompt redeposition agrees with measured net erosion within a factor of three. Sputtering by impurities, mainly boron, dominates erosion.
Plasma Physics and Controlled Fusion | 1995
Ian H. Hutchinson; B. LaBombard; Jennifer Ann Goetz; B. Lipschultz; G. McCracken; J. A. Snipes; J. L. Terry
Imbalances between the inboard and outboard legs of the single null divertor in tokamak Alcator C-Mod are observed to reverse when the direction of the toroidal field is reversed. These imbalances are measured by embedded probes in the target plates, tomographic reconstructions of bolometry and line radiation, and visible imaging. Density imbalances of about a factor of ten at the targets are observed at moderate density, decreasing as the density is raised until they are almost balanced. The data indicate that the electron pressure is not imbalanced, thus arguing against momentum imbalance as the cause of these drift-induced effects. Instead, power flux imbalance caused by Er V-product B convection, and enhanced by radiation, is suggested as the underlying cause.
Physics of Plasmas | 1996
J.A. Goetz; C. Kurz; B. LaBombard; B. Lipschultz; A. Niemczewski; G. McCracken; J. L. Terry; R. L. Boivin; F. Bombarda; P.T. Bonoli; C. Fiore; S. Golovato; R. Granetz; M. Greenwald; S. Horne; A. Hubbard; Ian H. Hutchinson; J. Irby; E. Marmar; M. Porkolab; J. E. Rice; J. A. Snipes; Y. Takase; R. Watterson; B. Welch; S. M. Wolfe; C. Christensen; D. Garnier; D. Jablonski; D. Lo
The divertor of the Alcator C‐Mod tokamak [Phys. Plasmas 1, 1511 (1994)] routinely radiates a large fraction of the power entering the scrape‐off layer. This dissipative divertor operation occurs whether the divertor is detached or not, and large volumetric radiative emissivities, up to 60 MW m−3 in ion cyclotron range of frequency (ICRF) heated discharges, have been measured using bolometer arrays. An analysis of both Ohmic and ICRF‐heated discharges has demonstrated some of the relative merits of detached divertor operation versus high‐recycling divertor operation. An advantage of detached divertor operation is that the power flux to the divertor plates is decreased even further than its already low value. Some disadvantages are that volumetric losses outside the separatrix in the divertor region are decreased, the neutral compression ratio is decreased, and the penetration efficiency of impurities increases.
Physics of Plasmas | 1995
B. L. Welch; Hans R. Griem; J. L. Terry; C. Kurz; B. LaBombard; B. Lipschultz; E. Marmar; G. McCracken
The electron density in the edge, divertor and X‐point regions of Alcator C‐Mod [Proceedings of the IEEE 13th Symposium on Fusion Engineering (Institute of Electrical and Electronic Engineers, New York, 1990), Vol. 1, p. 13] has been measured using the Stark broadening of high‐n (n=8 through 11) transitions of the Balmer series of deuterium. These measurements have been made during typical single null, diverted operation and during gas‐puffing through capillaries located within the first wall and divertor. Electron densities up to 1.6×1021 m−3 have been measured in the X‐point region and slightly lower densities (5−7×1020 m−3) have been measured in the divertor and edge regions. These results are factors of 2 to 5 larger than the density measurements from the CO2 laser interferometer system in the main chamber (3×1020 m−3) and comparable with probe measurements in the divertor. The ratios of the widths of adjacent lines within the Balmer series have been compared with ratios calculated for the Stark broad...
Physics of Plasmas | 2014
M. Greenwald; A. Bader; S. G. Baek; M. Bakhtiari; Harold Barnard; W. Beck; W. Bergerson; I.O. Bespamyatnov; P.T. Bonoli; D. L. Brower; D. Brunner; W. Burke; J. Candy; M. Churchill; I. Cziegler; A. Diallo; A. Dominguez; B.P. Duval; E. Edlund; P. Ennever; D. Ernst; I. Faust; C. Fiore; T. Fredian; O.E. Garcia; C. Gao; J.A. Goetz; T. Golfinopoulos; R. Granetz; O. Grulke
The object of this review is to summarize the achievements of research on the Alcator C-Mod tokamak [Hutchinson et al., Phys. Plasmas 1, 1511 (1994) and Marmar, Fusion Sci. Technol. 51, 261 (2007)] and to place that research in the context of the quest for practical fusion energy. C-Mod is a compact, high-field tokamak, whose unique design and operating parameters have produced a wealth of new and important results since it began operation in 1993, contributing data that extends tests of critical physical models into new parameter ranges and into new regimes. Using only high-power radio frequency (RF) waves for heating and current drive with innovative launching structures, C-Mod operates routinely at reactor level power densities and achieves plasma pressures higher than any other toroidal confinement device. C-Mod spearheaded the development of the vertical-target divertor and has always operated with high-Z metal plasma facing components—approaches subsequently adopted for ITER. C-Mod has made ground-breaking discoveries in divertor physics and plasma-material interactions at reactor-like power and particle fluxes and elucidated the critical role of cross-field transport in divertor operation, edge flows and the tokamak density limit. C-Mod developed the I-mode and the Enhanced Dα H-mode regimes, which have high performance without large edge localized modes and with pedestal transport self-regulated by short-wavelength electromagnetic waves. C-Mod has carried out pioneering studies of intrinsic rotation and demonstrated that self-generated flow shear can be strong enough in some cases to significantly modify transport. C-Mod made the first quantitative link between the pedestal temperature and the H-modes performance, showing that the observed self-similar temperature profiles were consistent with critical-gradient-length theories and followed up with quantitative tests of nonlinear gyrokinetic models. RF research highlights include direct experimental observation of ion cyclotron range of frequency (ICRF) mode-conversion, ICRF flow drive, demonstration of lower-hybrid current drive at ITER-like densities and fields and, using a set of novel diagnostics, extensive validation of advanced RF codes. Disruption studies on C-Mod provided the first observation of non-axisymmetric halo currents and non-axisymmetric radiation in mitigated disruptions. A summary of important achievements and discoveries are included.