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Featured researches published by J.S. Wrobel.


Nuclear Fusion | 2011

Recent results from the HIT-SI experiment

Thomas R. Jarboe; C. Akcay; M.A. Chilenski; D.A. Ennis; C.J. Hansen; N. Hicks; R.Z. Aboul Hosn; A.C. Hossack; G.J. Marklin; B.A. Nelson; R.G. O'Neill; P. E. Sieck; R.J. Smith; B.S. Victor; J.S. Wrobel; M. Nagata

New understanding and improved parameters have been achieved on the Helicity Injected Torus with Steady Inductive helicity injection current drive (HIT-SI) experiment. The experiment has a bowtie-shaped spheromak confinement region with two helicity injectors. The inductive injectors are 180° segments of a small, oval cross section toroidal pinch. Spheromaks with currents up to 38 kA and current amplification of 2 have been achieved with only 6 MW of injector power. The Taylor-state model is shown to agree with HIT-SI surface and internal magnetic profile measurements. Helicity balance predicts the peak magnitude of toroidal spheromak current and the threshold for spheromak formation. The model also accurately predicts the division of the applied loop voltage between the injector and spheromak regions. Single injector operation shows that the two injectors have opposing, preferred spheromak current directions. An electron locking relaxation model is consistent with the preferred direction, with ion Doppler data and with bolometric data. Results from higher frequency operation are given. The impact of the new understanding on the future direction of the HIT programme is discussed.


Nuclear Fusion | 2010

New understandings and achievements from independent-injector drive experiments on HIT-SI

D.A. Ennis; B.S. Victor; J.S. Wrobel; C. Akcay; Thomas R. Jarboe; G.J. Marklin; B.A. Nelson; R.J. Smith

The Helicity Injected Torus-Steady Inductive (HIT-SI) experiment investigates steady inductive helicity injection with the aim of forming and sustaining a high-beta equilibrium in a spheromak geometry using two semi-toroidal injectors. Results of experiments with unequal helicity injection rates produced the highest spheromak current (38kA), current amplification (Itor/Iinj quad ≈ 2) and poloidal flux amplification (ψpol/ψinj quad > 6) to date. Single-injectoroperationsestablishapreferreddirectionofgeneratedspheromakcurrentforeachinjectordepending on the sign of the injected helicity and its orientation relative to the confinement volume. Yet, the HIT-SI injectors prefer to drive opposing spheromak currents because they are mounted on opposite sides of the confinement volume. Single-injector operations also eliminate the spontaneous spheromak current flipping observed during dual-injector operations. PACS numbers: 52.55.Wq, 52.55.Ip (Some figures in this article are in colour only in the electronic version)


Physics of Plasmas | 2007

A fully relaxed helicity balance model for an inductively driven spheromak

R. G. O’Neill; G. J. Marklin; Thomas R. Jarboe; C. Akcay; W.T. Hamp; B.A. Nelson; Aaron John Redd; R.J. Smith; B. T. Stewart; J.S. Wrobel; P. E. Sieck

Magnetic helicity balance and a fully relaxed Taylor-state model are shown to predict the magnitude of sustained equilibrium current in an inductively driven spheromak. The Helicity Injected Torus with Steady Inductive drive (HIT-SI) [T. R. Jarboe et al., Phys. Rev. Lett. 97, 115003 (2006)] forms and sustains spheromaks using two inductively driven helicity injectors. By assuming helicity is injected at a rate 2VΨ, and only decays through Spitzer resistivity using Te measured with a Langmuir probe, the magnitude of the sustained equilibrium current is predicted with no fitting parameters. The model correctly predicts a threshold helicity injection rate for spheromak formation. Although the experimental results suggest a higher effective helicity dissipation rate by a factor of ∼1.37 compared to the Spitzer value, the prediction is still within the uncertainties of the measured parameters.


Physics of Plasmas | 2013

Relaxation-time measurement via a time-dependent helicity balance model

J.S. Wrobel; C.J. Hansen; Thomas R. Jarboe; Roger Smith; A.C. Hossack; B.A. Nelson; G.J. Marklin; D.A. Ennis; C. Akcay; B.S. Victor

A time-dependent helicity balance model applied to a spheromak helicity-injection experiment enables the measurement of the relaxation time during the sustainment phase of the spheromak. The experiment, the Helicity Injected Torus with Steady Inductive helicity injection (HIT-SI), studies spheromak formation and sustainment through inductive helicity injection. The model captures the dominant plasma behavior seen during helicity injection in HIT-SI by using an empirical helicity-decay rate, a time-dependent helicity-injection rate, and a composite Taylor state to model both the helicity content of the system and to calculate the resulting spheromak current. During single-injector operations, both the amplitude and the phase of the periodic rise and fall of the toroidal current are predicted by this model, with an exchange of helicity between the injector states and the spheromak state proposed as the causal mechanism. This phenomenon allows for the comparison of the delay between the current rises in the ...


Review of Scientific Instruments | 2013

Reduction of plasma density in the Helicity Injected Torus with Steady Inductance experiment by using a helicon pre-ionization source

A.C. Hossack; Taylor Firman; Thomas R. Jarboe; James Prager; B.S. Victor; J.S. Wrobel; Timothy Ziemba

A helicon based pre-ionization source has been developed and installed on the Helicity Injected Torus with Steady Inductance (HIT-SI) spheromak. The source initiates plasma breakdown by injecting impurity-free, unmagnetized plasma into the HIT-SI confinement volume. Typical helium spheromaks have electron density reduced from (2-3) × 10(19) m(-3) to 1 × 10(19) m(-3). Deuterium spheromak formation is possible with density as low as 2 × 10(18) m(-3). The source also enables HIT-SI to be operated with only one helicity injector at injector frequencies above 14.5 kHz. A theory explaining the physical mechanism driving the reduction of breakdown density is presented.


CURRENT TRENDS IN INTERNATIONAL FUSION RESEARCH: Proceedings of the 7th Symposium—Selected Presentations | 2009

SPHEROMAK FORMATION BY STEADY INDUCTIVE HELICITY INJECTION

Aaron John Redd; Thomas R. Jarboe; C. Akcay; R. Z. AboulHosn; W.T. Hamp; G.J. Marklin; B.A. Nelson; R. G. O’Neill; P. E. Sieck; R.J. Smith; B. T. Stewart; J.S. Wrobel

A spheromak is formed for the first time using a new steady state inductive helicity injection method. Using two inductive injectors with odd symmetry and oscillating at 5.8 kHz, a steady state spheromak with even symmetry is formed and sustained through nonlinear relaxation. A spheromak with about 13 kA of toroidal current is formed and sustained using about 3 MW of power. This is a much lower power threshold for spheromak production than required for electrode-based helicity injection. Internal magnetic probe data, including oscillations driven by the injectors, agree with the plasma being in the Taylor state. The agreement is remarkable considering the only fitting parameter is the amplitude of the spheromak component of the state.


Physical Review Letters | 2006

Spheromak formation by steady inductive helicity injection.

Thomas R. Jarboe; W.T. Hamp; G.J. Marklin; B.A. Nelson; R.G. O'Neill; Aaron John Redd; P. E. Sieck; R.J. Smith; J.S. Wrobel


Physical Review Letters | 2011

Evidence for separatrix formation and sustainment with steady inductive helicity injection.

B.S. Victor; Thomas R. Jarboe; A.C. Hossack; D.A. Ennis; B.A. Nelson; Roger Smith; C. Akcay; C.J. Hansen; G.J. Marklin; N. Hicks; J.S. Wrobel


Journal of Fusion Energy | 2007

Overview of HIT-SI Diagnostic Systems

R. G. O’Neill; R.J. Smith; C. Akcay; W.T. Hamp; R.Z. Aboul Hosn; T.R. Jarboe; Aaron John Redd; P. E. Sieck; G. L. Sutphin; J.S. Wrobel; Hit-Si Team


Journal of Fusion Energy | 2007

Overview of the Helicity Injected Torus (HIT) program

Aaron John Redd; T.R. Jarboe; W.T. Hamp; B.A. Nelson; R. G. O’Neill; P. E. Sieck; R.J. Smith; G. L. Sutphin; J.S. Wrobel

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B.A. Nelson

University of Washington

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T.R. Jarboe

University of Washington

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G.J. Marklin

University of Washington

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W.T. Hamp

University of Washington

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D.A. Ennis

University of Washington

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C. Akcay

Los Alamos National Laboratory

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B.S. Victor

University of Washington

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