R. O’Connell
University of Wisconsin-Madison
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Featured researches published by R. O’Connell.
Physics of Plasmas | 2002
Brett Edward Chapman; A. F. Almagri; J. K. Anderson; T. M. Biewer; P. K. Chattopadhyay; C.-S. Chiang; D. Craig; D.J. Den Hartog; G. Fiksel; Cary Forest; A. K. Hansen; D. Holly; Nicholas Edward Lanier; R. O’Connell; Stewart C. Prager; James Christian Reardon; J.S. Sarff; M. D. Wyman; D. L. Brower; W. X. Ding; Y. Jiang; S. D. Terry; P. Franz; L. Marrelli; P. Martin
Reduction of core-resonant m=1 magnetic fluctuations and improved confinement in the Madison Symmetric Torus [Dexter et al., Fusion Technol. 19, 131 (1991)] reversed-field pinch have been routinely achieved through control of the surface poloidal electric field, but it is now known that the achieved confinement has been limited in part by edge-resonant m=0 magnetic fluctuations. Now, through refined poloidal electric field control, plus control of the toroidal electric field, it is possible to reduce simultaneously the m=0 and m=1 fluctuations. This has allowed confinement of high-energy runaway electrons, possibly indicative of flux-surface restoration in the usually stochastic plasma core. The electron temperature profile steepens in the outer region of the plasma, and the central electron temperature increases substantially, reaching nearly 1.3 keV at high toroidal plasma current (500 kA). At low current (200 kA), the total beta reaches 15% with an estimated energy confinement time of 10 ms, a tenfold ...
Review of Scientific Instruments | 2008
J.A. Reusch; M. T. Borchardt; D.J. Den Hartog; A. F. Falkowski; D. J. Holly; R. O’Connell; H.D. Stephens
The multipoint Thomson scattering diagnostic on the Madison Symmetric Torus (MST) is now fully operational with 21 spatial points, which cover the entire minor radius. Four full electron temperature profiles can be obtained during each MST discharge, with a variable delay between each profile. This system overcomes challenges that arise from the unique machine design, location, and plasma characteristics of MST. The machine design limits the maximum porthole diameter to 11.4 cm, requiring a compact, re-entrant, seven element lens for scattered light collection. Limited space near MST necessitates a long beam path for the two Nd:YAG lasers requiring a remote beam line adjustment system to suppress drift in the beam position due to thermal expansion of the building. Due to the remote location of the laser head, substantial design effort was put into the creation of a set of safety interlocks for the laser system. The dynamic nature of MST plasmas and the wide range of operating space require a versatile scattered light detection system consisting of filter polychromators with temperature controlled avalanche photodiode detectors. We also implement an insertable integrating sphere, which travels along the laser beam path through the vacuum vessel, for the alignment of both the fiber optics and the lasers.
Physics of Plasmas | 2004
J. K. Anderson; T. M. Biewer; Cary Forest; R. O’Connell; Stewart C. Prager; J.S. Sarff
Transient application of a poloidal electric field to reversed field pinch (RFP) plasmas has led to a period in which dynamo activity (inherent in standard RFP plasmas) nearly vanishes. Measurements of the plasma resistivity, current density and electric field profiles show the edge-applied electric field accommodates Ohm’s law balance without a dynamo term over the entire cross section. Neoclassical theory accurately predicts the resistivity in the RFP, as the predicted resistivity profile (based on measurements of electron temperature, effective ionic charge, and two-dimensional equilibrium effects) is in agreement with the ratio of the parallel electric field and current density profiles.
Physics of Plasmas | 2005
J. K. Anderson; J. R. Adney; A. F. Almagri; Arthur Blair; D. L. Brower; M. Cengher; B.E. Chapman; S. Choi; D. Craig; Diane Renee Demers; D.J. Den Hartog; B.H. Deng; W. X. Ding; F. Ebrahimi; D.A. Ennis; G. Fiksel; Cary Forest; P. Franz; J.A. Goetz; Richard William Harvey; D. J. Holly; B. Hudson; M. C. Kaufman; Thomas W. Lovell; L. Marrelli; P. Martin; K.J. McCollam; V.V. Mirnov; Paul Nonn; R. O’Connell
Generation and sustainment of the reversed field pinch (RFP) magnetic configuration normally relies on dynamo activity. The externally applied electric field tends to drive the equilibrium away from the relaxed, minimum energy state which is roughly described by a flat normalized parallel current density profile and is at marginal stability to tearing modes. Correlated fluctuations of magnetic field and velocity create a dynamo electric field which broadens the parallel current density profile, supplying the necessary edge current drive. These pervasive magnetic fluctuations are also responsible for destruction of flux surfaces, relegating the standard RFP to a stochastic-magnetic transport-limited device. Application of a tailored electric field profile (which matches the relaxed current density profile) allows sustainment of the RFP configuration without dynamo-driven edge current. The method used to ascertain that a dynamo-free RFP plasma has been created is reported here in detail. Several confinement...
Review of Scientific Instruments | 2003
R. O’Connell; D.J. Den Hartog; Cary Forest; R. W. Harvey
A 16 spatial channel hard x-ray (HXR) diagnostic using solid state CdZnTe detectors (active area 10 mm×10 mm×2 mm, 50 mm×20 mm×20 mm packaged) has recently been installed on the Madison Symmetric Torus (MST) reversed field pinch to measure the XR flux from ∼10 to 300 keV. Rather than using conventional pulse height analysis, the shaped output pulses from the detector are digitized using 12-bit, 10 MHz ADCs. The resulting waveforms are then fitting with multiple Gaussians; this allows a fraction of normally discarded pile-up events to be recovered. The technique is cost effective and allows for (a) excellent energy resolution—limited by the detector resolution rather than electronics; (b) dynamic time binning—rather than counting over predefined time bins, x-ray events are recorded as discretely timed events; (c) better noise rejection/pile up detection—achieved by fitting using the full information of the time history and known pulse shape from the amplifier; and (d) simple hardware implementation. The me...
Review of Scientific Instruments | 2008
R. O’Connell; D.J. Den Hartog; M. T. Borchardt; D. J. Holly; J.A. Reusch; H.D. Stephens
The Madison Symmetric Torus (MST) presents challenging conditions for Thomson scattering (TS) measurements. The MST plasmas are reversed-field pinches (RFPs) with electron density n(e)<3x10(13) cm(-3), typically 1x10(13) cm(-3). The TS system was designed to measure from 10 eV to 2 keV; however, six polychromators were upgraded from four to eight spectral channels to resolve to 10 keV. There is no diverter or vertical field, so wall interaction results in high background light both from ion and neutral bremsstrahlungs and from line radiation. Also during standard plasmas, the RFP exhibits regular reconnection sawteeth events during which the plasma current, density, and temperature profiles are flattened. These events are of interest both due to the reconnection physics and to their contribution to the MST equilibrium and confinement. These events occur over 100 microS and exhibit large changes in background light and fast changes in temperature. During improved confinement plasmas, there are no sawteeth; the background is low but the temperature can be over an order of magnitude higher. Data analysis of the system has been developed to accommodate both the large dynamic range of the temperature, the fast dynamics, and the fast changing, high amplitude background. Special attention has been paid to the sources of error, in particular, the contribution of the background. A response-function method reduces the measured uncertainty by a factor of 2. Numerical techniques have been developed which are extremely robust. Two methods are used, a conventional chi(2) minimization using a Levenberg-Marquardt algorithm coupled with Monte Carlo modeling for the error bar and a Bayesian statistics method. The Bayesian method computes the probability distribution for the measured photons and electron temperature and this information can be used to ensemble data and will allow future integrated data analysis efforts.
Review of Scientific Instruments | 2008
H.D. Stephens; M. T. Borchardt; D.J. Den Hartog; A. F. Falkowski; D. J. Holly; R. O’Connell; J.A. Reusch
Detailed calibrations of the Madison Symmetric Torus polychromator Thomson scattering system have been made suitable for electron temperature fluctuation measurements. All calibrations have taken place focusing on accuracy, ease of use and repeatability, and in situ measurements wherever possible. Novel calibration processes have been made possible with an insertable integrating sphere (ISIS), using an avalanche photodiode (APD) as a reference detector and optical parametric oscillator (OPO). Discussed are a novel in situ spatial calibration with the use of the ISIS, the use of an APD as a reference detector to streamline the APD calibration process, a standard dc spectral calibration, and in situ pulsed spectral calibration made possible with a combination of an OPO as a light source, the ISIS, and an APD used as a reference detector. In addition a relative quantum efficiency curve for the APDs is obtained to aid in uncertainty analysis.
Physics of Plasmas | 2004
S. D. Terry; D. L. Brower; W. X. Ding; J. K. Anderson; T. M. Biewer; Brett Edward Chapman; D. Craig; Cary Forest; R. O’Connell; Stewart C. Prager; J.S. Sarff
The current profile and core magnetic field fluctuation amplitudes in a reversed-field pinch are measured by using a high-resolution polarimetry–interferometry system. This paper presents data showing a redistribution of the current during a sawtooth crash. Also, the core magnetic field fluctuation amplitude is observed to increase at a sawtooth crash consistent with the idea of nonlinearly driven dynamo current. In addition, the parallel current density increases in the outer region of the plasma during auxiliary pulsed parallel current drive. This was expected, as the external application of an edge parallel electric field is designed to flatten the current profile providing an equilibrium closer to the minimum energy Taylor state. However, the current density also increases in the core, relative to standard plasmas. This increase can be explained by a reduction of the dynamo (anti)current drive in the core that should accompany the measured reduction of magnetic fluctuations and by a drop in resistivity caused by the increased confinement of fast electrons.
Review of Scientific Instruments | 2006
P. Franz; F. Bonomo; L. Marrelli; Piero Martin; P. Piovesan; G. Spizzo; B.E. Chapman; D. Craig; D.J. Den Hartog; J.A. Goetz; R. O’Connell; Stewart C. Prager; M. Reyfman; J.S. Sarff
Two-dimensional (2D) time resolved images of the electron temperature profile in the core of the MST reversed field pinch plasma are presented. The measurements have been obtained with a soft x-ray (SXR) tomographic diagnostic comprised of four cameras, each with a multichannel photodiode array, viewing the plasma at different poloidal angles, with a total of 74 channels. The 2D electron temperature profile is estimated by simultaneously measuring the SXR emissivity through different beryllium foils, using the standard double-filter technique. With these methods, fast temperature variation in the core of the plasma (up to 100kHz) can be analyzed.
Physics of Plasmas | 2010
K.J. McCollam; J. K. Anderson; Arthur Blair; D. Craig; D.J. Den Hartog; F. Ebrahimi; R. O’Connell; J.A. Reusch; J.S. Sarff; H.D. Stephens; D.R. Stone; D. L. Brower; B.H. Deng; W. X. Ding
Oscillating-field current drive (OFCD) is a proposed method of steady-state toroidal plasma sustainment in which ac poloidal and toroidal loop voltages are applied to produce a dc plasma current. OFCD is added to standard, inductively sustained reversed-field pinch plasmas in the Madison Symmetric Torus [R. N. Dexter et al., Fusion Technol. 19, 131 (1991)]. Equilibrium profiles and fluctuations during a single cycle are measured and analyzed for different relative phases between the two OFCD voltages and for OFCD off. For OFCD phases leading to the most added plasma current, the measured energy confinement is slightly better than that for OFCD off. By contrast, the phase of the maximum OFCD helicity-injection rate also has the maximum decay rate, which is ascribed to transport losses during discrete magnetic-fluctuation events induced by OFCD. Resistive-magnetohydrodynamic simulations of the experiments reproduce the observed phase dependence of the added current.