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Dive into the research topics where K.J. McCollam is active.

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Featured researches published by K.J. McCollam.


Nuclear Fusion | 2003

Tokamak-like confinement at a high beta and low toroidal field in the MST reversed field pinch

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 | 2002

Current drive experiments in the helicity injected torus (HIT-II)

Aaron John Redd; B.A. Nelson; T.R. Jarboe; P. Gu; R. Raman; Roger Smith; K.J. McCollam

The Helicity Injected Torus [HIT-II: T. Jarboe et al., Phys. Plasmas 5, 1807 (1998)] is a low-aspect-ratio tokamak capable of both inductive (ohmic) and Coaxial Helicity Injection (CHI) current drive. HIT-II is modest in size (major radius R=0.3 m, minor radius a=0.2 m, and on-axis toroidal field of up to 0.5 T), but has demonstrated 200 kA of toroidal plasma current, using either CHI or induction separately. The loop voltage, boundary flux, and plasma equilibrium are controlled by a real-time flux feedback system. HIT-II ohmic plasmas exhibit reconnection events during both the current ramp-up and decay, events that relax the current profile while conserving the magnetic helicity. A new operating regime for CHI plasmas, using a double-null divertor (DND) boundary flux, has been explored. DND CHI plasmas exhibit good shot-to-shot reproducibility, low impurity content, minimal shorting current in the absorber region, and EFIT-reconstructed equilibria consistent with significant closed-flux core regions [EF...


Nuclear Fusion | 2009

Overview of RFX-mod results

P. Martin; L. Apolloni; M. E. Puiatti; J. Adamek; M. Agostini; A. Alfier; Silvia Valeria Annibaldi; V. Antoni; F. Auriemma; O. Barana; M. Baruzzo; P. Bettini; T. Bolzonella; D. Bonfiglio; M. Brombin; J. Brotankova; A. Buffa; Paolo Buratti; A. Canton; S. Cappello; L. Carraro; R. Cavazzana; M. Cavinato; B.E. Chapman; G. Chitarin; S. Dal Bello; A. De Lorenzi; G. De Masi; D. F. Escande; A. Fassina

With the exploration of the MA plasma current regime in up to 0.5 s long discharges, RFX-mod has opened new and very promising perspectives for the reversed field pinch (RFP) magnetic configuration, and has made significant progress in understanding and improving confinement and in controlling plasma stability. A big leap with respect to previous knowledge and expectations on RFP physics and performance has been made by RFX-mod since the last 2006 IAEA Fusion Energy Conference. A new self-organized helical equilibrium has been experimentally achieved (the Single Helical Axis—SHAx—state), which is the preferred state at high current. Strong core electron transport barriers characterize this regime, with electron temperature gradients comparable to those achieved in tokamaks, and by a factor of 4 improvement in confinement time with respect to the standard RFP. RFX-mod is also providing leading edge results on real-time feedback control of MHD instabilities, of general interest for the fusion community.


Plasma Physics and Controlled Fusion | 2008

High current regimes in RFX-mod

M. Valisa; T. Bolzonella; P. Buratti; L. Carraro; R. Cavazzana; S. Dal Bello; P. Martin; R. Pasqualotto; J.S. Sarff; M. Spolaore; P. Zanca; L. Zanotto; M. Agostini; A. Alfier; V. Antoni; L. Apolloni; F. Auriemma; O. Barana; M. Baruzzo; P. Bettini; D. Bonfiglio; M. Brombin; A. Buffa; A. Canton; S. Cappello; M. Cavinato; G. Chitarin; A. De Lorenzi; G. De Masi; D. F. Escande

Optimization of machine operation, including plasma position control, density control and especially feedback control on multiple magnetohydrodynamic modes, has led RFX-mod to operate reliably at 1.5?MA, the highest current ever achieved on a reversed field pinch (RFP). At high current and low density the magnetic topology spontaneously self-organizes in an Ohmical helical symmetry, with the new magnetic axis helically twisting around the geometrical axis of the torus. The separatrix of the island disappears leaving a wide and symmetric thermal structure with large gradients in the electron temperature profile. The new topology still displays an intermittent nature but its overall presence has reached 85% of the current flat-top period. The large gradients in the electron temperature profile appear to be marginal for the destabilization of ion temperature gradient modes on the assumption that ions and electrons have the same gradients. There are indications that higher currents could provide the conditions under which to prove the existence of a true helical equilibrium as the standard RFP configuration.


Review of Scientific Instruments | 2004

Compact high-resolution ion Doppler spectrometer for quartz ultraviolet line emissions

Peimin Gu; M. Nagata; K.J. McCollam; Thomas R. Jarboe; B.A. Nelson; Aaron John Redd

A high-resolution quartz ultraviolet spectrometer based on a single compact 16-channel multianode photomultiplier tube (MAPMT) has been developed and tested on coaxial helicity injection and ohmic transformer current drive plasmas generated on the Helicity Injected Torus at the University of Washington. The use of the compact MAPMT allows a simple design with high light collection and high resolution for an ion Doppler shift diagnostic. The high quality and low cost of the design make it uniquely attractive for university scale plasma experiments. The Doppler shift of impurity ion emission lines from two chords of equal impact parameter but of opposite rotational sense is used to determine chord-averaged toroidal flow velocity. The width of the Doppler broadening is used to calculate the ion temperature. A detailed description of the ion Doppler spectrometer measurement system and some typical results are presented.


Physics of Plasmas | 2005

Dynamo-free plasma in the reversed-field pinch : Advances in understanding the reversed-field pinch improved confinement mode

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

Overview of results in the MST reversed field pinch experiment

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.


Plasma Physics and Controlled Fusion | 2015

Control of 3D equilibria with resonant magnetic perturbations in MST

S. Munaretto; B.E. Chapman; D. J. Holly; M. D. Nornberg; Ryan Norval; D.J. Den Hartog; J.A. Goetz; K.J. McCollam

To aid in diagnosis of 3D equilibria in the Madison Symmetric Torus, it has become necessary to control the orientation of the equilibria. In reversed field pinch experiments a transition to a 3D equilibrium is common with sufficiently large plasma current (and Lundquist number). Diagnosis of this state is hampered by the fact that the helical structure is stationary but with an orientation that varies shot-to-shot. A resonant magnetic perturbation (RMP) technique has been developed to vary controllably the orientation of the 3D equilibria and optimized to minimize the plasma wall interaction due to its use. Application of an RMP now allows alignment of the structure with key diagnostics, including Thomson scattering and an interferometer-polarimeter.


Physics of Plasmas | 2010

Equilibrium evolution in oscillating-field current-drive experiments

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.


Plasma Physics and Controlled Fusion | 2008

Internal magnetic field structure and parallel electric field profile evolution during the sawtooth cycle in MST

B.H. Deng; W. X. Ding; D. L. Brower; A. F. Almagri; K.J. McCollam; Y Ren; Stewart C. Prager; J.S. Sarff; J.A. Reusch; J. K. Anderson

Temporal dynamics of the magnetic field, parallel current density, parallel electric field and safety factor profiles in the core of a high-temperature reversed-field pinch plasma are experimentally resolved. Measurements are realized using a high-speed polarimeter–interferometer diagnostic which is employed to simultaneously determine the electron density, toroidal current density and poloidal magnetic field profiles. Combined with external magnetic measurements, these data allow determination of the equilibrium profile dynamics during individual sawtooth magnetic relaxation events. At the sawtooth crash, the E∥ profile has a large positive peak on-axis, and a negative peak of slightly smaller value near the reversal surface demonstrating the need for a dynamo to sustain the plasma equilibrium.

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J.S. Sarff

University of Wisconsin-Madison

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A. F. Almagri

University of Wisconsin-Madison

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B.E. Chapman

University of Wisconsin-Madison

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D. Craig

University of Wisconsin-Madison

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D.J. Den Hartog

University of Wisconsin-Madison

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Stewart C. Prager

University of Wisconsin-Madison

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Arthur Blair

University of Wisconsin-Madison

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W. X. Ding

University of California

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D. L. Brower

University of California

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