Arthur Blair
University of Wisconsin-Madison
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Featured researches published by Arthur Blair.
Nuclear Fusion | 2003
J.S. Sarff; A. F. Almagri; J. K. Anderson; T. M. Biewer; Arthur Blair; M. Cengher; Brett Edward Chapman; P. K. Chattopadhyay; D. Craig; D.J. Den Hartog; F. Ebrahimi; G. Fiksel; Cary Forest; J.A. Goetz; D. J. Holly; B. Hudson; Thomas W. Lovell; K.J. McCollam; Paul Nonn; R. O'Connell; S. P. Oliva; Stewart C. Prager; James Christian Reardon; Mike Thomas; M. D. Wyman; D. L. Brower; W. X. Ding; S. D. Terry; Mark Dwain Carter; V. I. Davydenko
Energy confinement comparable with tokamak quality is achieved in the Madison Symmetric Torus (MST) reversed field pinch (RFP) at a high beta and low toroidal magnetic field. Magnetic fluctuations normally present in the RFP are reduced via parallel current drive in the outer region of the plasma. In response, the electron temperature nearly triples and beta doubles. The confinement time increases ten-fold (to ~10 ms), which is comparable with L- and H-mode scaling values for a tokamak with the same plasma current, density, heating power, size and shape. Runaway electron confinement is evidenced by a 100-fold increase in hard x-ray bremsstrahlung. Fokker–Planck modelling of the x-ray energy spectrum reveals that the high energy electron diffusion is independent of the parallel velocity, uncharacteristic of magnetic transport and more like that for electrostatic turbulence. The high core electron temperature correlates strongly with a broadband reduction of resonant modes at mid-radius where the stochasticity is normally most intense. To extend profile control and add auxiliary heating, rf current drive and neutral beam heating are in development. Low power lower-hybrid and electron Bernstein wave injection experiments are underway. Dc current sustainment via ac helicity injection (sinusoidal inductive loop voltages) is also being tested. Low power neutral beam injection shows that fast ions are well-confined, even in the presence of relatively large magnetic fluctuations.
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...
Nuclear Fusion | 2005
Stewart C. Prager; J. R. Adney; A. F. Almagri; J. K. Anderson; Arthur Blair; D. L. Brower; M. Cengher; B.E. Chapman; S. Choi; D. Craig; S.K. Combs; Diane Renee Demers; D.J. Den Hartog; B.H. Deng; W. X. Ding; F. Ebrahimi; D.A. Ennis; G. Fiksel; Richard Fitzpatrick; C.R. Foust; Cary Forest; P. Franz; L. Frassinetti; J.A. Goetz; D. J. Holly; B. Hudson; M. C. Kaufman; Thomas W. Lovell; L. Marrelli; P. Martin
Confinement in the reversed field pinch (RFP) has been shown to increase strongly with current profile control. The MST RFP can operate in two regimes: the standard regime with a naturally occurring current density profile, robust reconnection and dynamo activity; and the improved confinement regime with strong reduction in reconnection, dynamo and transport. New results in standard plasmas include the observation of a strong two-fluid Hall effect in reconnection and dynamo, the determination that the m = 0 edge resonant mode is nonlinearly driven, and the determination that tearing modes can lock to the wall via eddy currents in the shell. New results in improved confinement plasmas include observations that such plasmas are essentially dynamo-free, contain several isolated magnetic islands (as opposed to a stochastic field) and contain reduced high frequency turbulence. Auxiliary current drive and heating is now critical to RFP research. In MST, a programme to apply auxiliary systems to the RFP is underway and progress has accrued in several techniques, including lower hybrid and electron Bernstein wave injection, ac helicity injection current drive, pellet injection and neutral beam injection.
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.
Nuclear Fusion | 2007
D.J. Den Hartog; J. W. Ahn; A. F. Almagri; J. K. Anderson; A. D. Beklemishev; Arthur Blair; M. T. Borchardt; D. L. Brower; D. R. Burke; M. Cengher; B.E. Chapman; S. Choi; D.J. Clayton; W.A. Cox; S.K. Combs; D. Craig; H. D. Cummings; V. I. Davydenko; Diane Renee Demers; B.H. Deng; W. X. Ding; F. Ebrahimi; D.A. Ennis; G. Fiksel; C.R. Foust; Cary Forest; P. Franz; L. Frassinetti; S. Gangadhara; J.A. Goetz
In the general area of confinement improvement and concept advancement, recent results in the Madison Symmetric Torus (MST) reversed-field pinch (RFP) include good confinement of both thermal and large-orbit ions and near doubling of total beta to 26% with deuterium pellet injection. Current profile control enables MST to reduce stochastic transport and achieve tokamak-like confinement. In standard RFP operation, substantial MHD tearing mode activity results in stochastic transport and an energy confinement time of about 1 ms in MST. Application of inductive current profile control reduces MHD activity and accompanying stochasticity, improving confinement by about a factor of ten. Previous work concentrated on electron confinement in improved-confinement RFP operation. Recent work confirms that ions are also well confined, and that high beta and improved confinement can be achieved simultaneously. PACS numbers: 52.55.Hc, 52.55.Dy (Some figures in this article are in colour only in the electronic version)
Review of Scientific Instruments | 2011
Paul Nonn; Arthur Blair; K.J. McCollam; J.S. Sarff; D.R. Stone
A 10-MVA-scale resonant oscillator, powered by a pulse-forming network and switched with a pair of commutating mercury ignitrons, was developed for the MST reversed-field pinch plasma-confinement experiment. A novel feature of this circuit is its commutation mechanism, wherein each turning on of one ignitron causes a reverse voltage transient that turns off the other. Two of these oscillators are used in oscillating-field current-drive tests, in which they are capable of nearly 1MW net input power to the plasma, with resonant frequencies of a few 100 Hz for pulse durations of a few tens of ms, being precharged for immediate full amplitude. We describe the circuit and its operation, and discuss features that allow reliable, high-current commutation of the ignitrons and exploit their low switching impedance.
Physical Review Letters | 2006
K.J. McCollam; Arthur Blair; Stewart C. Prager; J.S. Sarff
CURRENT TRENDS IN INTERNATIONAL FUSION RESEARCH: Proceedings of the 7th Symposium—Selected Presentations | 2009
K.J. McCollam; J. K. Anderson; Arthur Blair; B.E. Chapman; D. Craig; D.J. Den Hartog; F. Ebrahimi; G. Fiksel; S. Gangadhara; J.A. Goetz; B. Hudson; R. O’Connell; Stewart C. Prager; J. Sarff; M. D. Wyman; Mst Team
Bulletin of the American Physical Society | 2006
K.J. McCollam; Arthur Blair; F. Ebrahimi; Paul Nonn; J.S. Sarff; A. F. Almagri; Jay Anderson; D. Craig; D.J. Den Hartog; G. Fiksel; S. Gangadhara; R. O'Connell; Stewart C. Prager; B.H. Deng; W. X. Ding; D. L. Brower
32nd European Physical Society Conference on Plasma Physics and Controlled Fusion combined with the 8th International Workshop on Fast Ignition of Fusion Targets | 2005
J.A. Goetz; J. K. Anderson; Arthur Blair; M. Cengher; G. Fiksel; Cary Forest; B. Hudson; M. C. Kaufman; K.J. McCollam; Stewart C. Prager; J.S. Sarff; Mike Thomas