R.C. Isler
Oak Ridge National Laboratory
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Featured researches published by R.C. Isler.
Plasma Physics and Controlled Fusion | 1994
R.C. Isler
Charge-exchange spectroscopy in fusion plasmas entails the use of optical transitions that follow electron transfer from a neutral atom into an excited state of an impurity ion. In most applications, the sources of neutral particles are high-energy beams employed either for heating or for the specific purpose of active plasma diagnosis. The transitions following charge exchange are particularly useful for determining the densities of fully stripped low-Z ions and for measuring ion temperatures and plasma rotation, although they have also been exploited for other purposes. In this review, the atomic physics considerations for interpreting the data, including the influence of the plasma environment, are reviewed, and examples of recent applications to fusion studies are presented.
Nuclear Fusion | 1984
R.C. Isler
Impurities continue to be a concern for future fusion devices, and ongoing efforts are made to study their generation, confinement, and control. Techniques for analysis of concentrations, power losses, and confinement of impurities are surveyed, and experimental examples illustrating typical observations in tokamak plasmas are presented. The use of impurities for diagnosing plasma properties is outlined briefly.
Physics of Plasmas | 1997
R.C. Isler; G. R. McKee; N. H. Brooks; W.P. West; M.E. Fenstermacher; R. D. Wood
Thomson scattering measurements performed in the divertor of the DIII-D tokamak [Plasma Physics Controlled Nuclear Fusion Research, 1986 (International Atomic Energy Agency, Vienna, 1987), Vol. I, p. 159] during detached operation show that the electron temperatures are typically between 0.8 and 2.0 eV throughout a region which may extend several centimeters above the target plate. At such low temperatures the excitation of recycling deuterium atoms or impurities should be weak. Nevertheless, significant radiation is frequently detected in these locations. It has been suggested that recombination processes, which become important only below about 1.5 eV for deuterium, are responsible for the observed emission. This hypothesis has been investigated by comparing ratios of deuterium lines from attached and detached plasmas with theoretical ratios expected for ionizing or recombining conditions. The analysis of several discharges indicates that the mechanism for production of the emission changes from being c...
Nuclear Fusion | 1981
R.M. Gilgenbach; M.E. Read; K.E. Hackett; R.F. Lucey; V.L. Granatstein; A.C. England; C.M. Loring; J. B. Wilgen; R.C. Isler; Y-K.M. Peng; K.H. Burrell; O.C. Eldridge; M.P. Hacker; P.W. King; A.G. Kulchar; M. Murakami; R.K. Richards
Pre-ionization experiments have been performed on a tokamak by injecting about 80 kW of microwave power at 35 GHz for up to 15 ms. Microwave absorption occurs at the electron cyclotron and upper hybrid resonance frequencies as predicted by theory. Pre-ionization causes substantial (40%) reductions in loop voltage during the initial phase of the tokamak shot. Flux (volt-second) savings with pre-ionization are about 30% in the first 2 ms or about 2% of the total flux expenditure in a tokamak shot. The plasma current begins 200 μs earlier and rises 1.4 times more rapidly in the pre-ionized case. Electron densities of 5 × 1012 cm−3 can be sustained throughout the microwave pulse with only a toroidal magnetic field during microwave injection. The bulk electron temperature in the pre-ionized plasma is about 10 eV although there are indications of higher electron temperatures (50 eV) in the upper hybrid resonance layer. Although questions exist concerning the quiescent behaviour of the pre-ionized plasma, the observed parameters are shown to be consistent with a theory which employs classical models of energy and particle balance. During the early stages of Ohmic heating, the pre-ionization is effective in decreasing the peak of the radiated power.
Journal of Nuclear Materials | 2003
P.C. Stangeby; J.D. Elder; J.A. Boedo; B.D. Bray; N. H. Brooks; M.E. Fenstermacher; M. Groth; R.C. Isler; L.L. Lao; S. Lisgo; G.D. Porter; D. Reiter; D.L. Rudakov; J.G. Watkins; W.P. West; D.G. Whyte
Abstract Recently a number of major, unanticipated effects have been reported in tokamak edge research raising the question of whether we understand the controlling physics of the edge. This report is on the first part – here focused on the outer divertor – of a systematic study of the simplest possible edge plasma – no ELMs, no detachment, etc. – for a set of 10 repeat, highly diagnosed, single-null, divertor discharges in DIII-D. For almost the entire, extensive data set so far evaluated, the matches of experiment and model are so close as to imply that the controlling processes at the outer divertor for these simple plasma conditions have probably been correctly identified and quantitatively characterized in the model. The principal anomaly flagged so far relates to measurements of Te near the target, potentially pointing to a deficiency in our understanding of sheath physics in the tokamak environment.
Nuclear Fusion | 1983
R.C. Isler; L.E. Murray; E.C. Crume; C.E. Bush; J.L. Dunlap; P.H. Edmonds; S. Kasai; E. A. Lazarus; M. Murakami; G.H. Neilson; V.K. Paré; S.D. Scott; C.E. Thomas; A.J. Wootton
Recent calculations have shown that when external momentum sources and plasma rotation are included in the neoclassical theory, the standard results for impurity transport can be strongly altered. Under appropriate conditions, inward convection is reduced by co-injection and enhanced by counter-injection. In order to examine the theoretical predictions, several observations of impurity transport have been made in the ISX-B tokamak during neutral-beam injection for comparison with the transport seen with Ohmic heating alone. Both intrinsic contaminants and deliberately introduced test impurities display a behaviour that is in qualitative agreement with the predicted beam-driven effects. These correlations are particularly noticeable when the comparisons are made for deuterium where the impurity transport in the Ohmically heated discharges exhibits neoclassical-like characteristics, i.e. accumulation and long confinement times. Similar but smaller effects are observed in beam-heated hydrogen discharges; neoclassical-like behaviour is not seen in Ohmically heated hydrogen sequences. Emphasis has been placed on measuring toroidal plasma rotation, and semi-quantitative comparisons with the theories of beam-induced impurity transport have been made. It is possible that radial electric fields other than those associated with momentum transfer and increased anomalous processes during injection could also play a role.
Physics of Plasmas | 1997
R.C. Isler; R. W. Wood; C. C. Klepper; N. H. Brooks; M.E. Fenstermacher; A.W. Leonard
Radiative losses along a fixed view into the divertor chamber of the DIII-D tokamak [Plasma Physics Controlled Nuclear Fusion Research 1986 (International Atomic Energy Agency, Vienna, 1987), Vol I, p. 159] have been characterized for attached and partially detached discharges by analyzing line-integrated vacuum ultraviolet (VUV) signals. Essentially all the emission can be ascribed to carbon and deuterium. Because the majority of the most intense lines, which lie at wavelengths above 1100 A, are not accessible to the present instrumentation, extensive use has been made of collisional-radiative (CR) calculations for level populations of the important ions in order to relate the total radiated power to shorter wavelength transitions. In beam-heated plasmas, the fraction of radiation detected from carbon along the VUV spectrometer view is usually between 50% and 80% of the total. Carbon densities are estimated from a simplified approach to modelling the emission using a one-dimensional transport code. For p...
Nuclear Fusion | 1986
P.K. Mioduszewski; P.H. Edmonds; C.E. Bush; A. Carnevali; R.E. Clausing; T.B. Cook; L.C. Emerson; A.C. England; W.A. Gabbard; L. Heatherly; D. P. Hutchinson; R.C. Isler; R.R. Kindsfather; P.W. King; R.A. Langley; E. A. Lazarus; C.H. Ma; M. Murakami; G.H. Neilson; J.B. Roberto; J. E. Simpkins; C.E. Thomas; A.J. Wootton; K. Yokoyama; R. A. Zuhr; K.H. Behringer; J. Dietz; E. Källne; P.J. Lomas; P.D. Morgan
An experiment to test beryllium as a limiter material has been performed in the ISX-B tokamak. The effect of the plasma on the limiter and the effect of the limiter on the plasma were studied in detail. Heat and particle fluxes to the limiter were measured, and limiter damage by melting was documented as a function of power flux. Strong melting and evaporation of the limiter caused beryllium gettering of the vacuum vessel. Postmortem analysis of the limiter was performed to document the amount of retained hydrogen and the erosion and impurity deposition on the limiter. The effect of the limiter on the plasma performance was studied in terms of parameter space, impurity content, and confinement for the ungettered and gettered cases. Operational experience with beryllium in a fusion experiment is discussed.
Nuclear Fusion | 2002
M.A. Mahdavi; T.H. Osborne; A.W. Leonard; M. S. Chu; E. J. Doyle; M.E. Fenstermacher; G.R. McKee; G. M. Staebler; T.W. Petrie; M.R. Wade; S.L. Allen; J.A. Boedo; N. H. Brooks; R.J. Colchin; T.E. Evans; C. M. Greenfield; G.D. Porter; R.C. Isler; R.J. La Haye; C.J. Lasnier; R. Maingi; R.A. Moyer; Michael J. Schaffer; P.G. Stangeby; J.G. Watkins; W.P. West; D.G. Whyte; Nancy Wolf
Densities of up to 40% above the Greenwald limit are reproducibly achieved in high confinement (HITER89P = 2) ELMing H mode discharges. Simultaneous gas fuelling and divertor pumping were used to obtain these results. Confinement of these discharges, similar to moderate density H mode, is characterized by a stiff temperature profile, and is therefore sensitive to the density profile. A particle transport model is presented that explains the roles of divertor pumping and geometry for access to high densities. The energy loss per ELM at high density is a factor of five lower than the predictions of an earlier scaling, based on data from lower density discharges.
Journal of Nuclear Materials | 1984
E. A. Lazarus; J.D. Bell; C.E. Bush; A. Carnevali; J.L. Dunlap; P.H. Edmonds; L.C. Emerson; O.C. Eldridge; W.L. Gardner; H.C. Howe; D. P. Hutchinson; R.R. Kindsfather; R.C. Isler; R.A. Langley; C.H. Ma; P.K. Mioduszewski; M. Murakami; L.E. Murray; G.H. Neilson; V.K. Paré; S.D. Scott; D.J. Sigmar; J.E. Simpkins; K.A. Stewart; C.E. Thomas; R.M. Wieland; J. B. Wilgen; A.L. Wintenberg; W.R. Wing; A.J. Wootton
Abstract Results are reported on improved confinement in the Impurity Study Experiment (ISX-B) neutral beam heated plasmas when a small amount of neon is injected shortly after the start of beam heating. The scaling of energy confinement is modified by the introduction of a dependence on line-averaged density. Calculations show the improvement is primarily caused by a reduction in electron heat conduction.