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Featured researches published by S. Angelini.
Physics of Plasmas | 2013
D. Shiraki; S. Angelini; P.J. Byrne; B. DeBono; P.E. Hughes; J.P. Levesque; M.E. Mauel; D.A. Maurer; Gerald A. Navratil; Q. Peng; N. Rath; D.J. Rhodes; C.C. Stoafer
The detailed measurements of the 3D plasma response to applied external magnetic perturbations in the presence of a rotating external kink are presented, and compared with the predictions of a single-helicity linear model of kink mode dynamics. The modular control coils of the High Beta Tokamak-Extended Pulse (HBT-EP) device are used to apply resonant m/n = 3/1 magnetic perturbations to wall-stabilized tokamak plasmas with a pre-existing rotating 3/1 kink mode. The plasma response is measured in high-resolution with the extensive magnetic diagnostic set of the HBT-EP device. The spatial structures of both the naturally rotating kink mode and the externally driven response are independently measured and observed to be identical, while the temporal dynamics are consistent with the independent evolution and superposition of the two modes. This leads to the observation of a characteristic change in 3D field dynamics as a function of the applied field amplitude. This amplitude dependence is found to be different for poloidal and radial fields. The measured 3D response is compared to and shown to be consistent with the predictions of the linear single-helicity model in the “high-dissipation” regime, as reported previously [M. E. Mauel et al., Nucl. Fusion 45, 285 (2005)].
Physics of Plasmas | 2012
D.A. Maurer; D. Shiraki; J.P. Levesque; James M. Bialek; S. Angelini; P.J. Byrne; B. DeBono; P.E. Hughes; M.E. Mauel; Gerald A. Navratil; Q. Peng; Dov Rhodes; Nickolaus Rath; C.C. Stoafer
We report high-resolution detection of the 3D plasma magnetic response of wall-stabilized tokamak discharges in the High Beta Tokamak-Extended Pulse [T. H. Ivers et al., Phys. Plasmas 3, 1926 (1996)] device. A new adjustable conducting wall has been installed on HBT-EP made up of 20 independent, movable, wall segments instrumented with three distinct sets of 40 modular coils that can be independently driven to generate a wide variety of magnetic perturbations. High-resolution detection of the plasma response is made with 216 poloidal and radial magnetic sensors that have been located and calibrated with high-accuracy. Static and dynamic plasma responses to resonant and non-resonant magnetic perturbations are observed through measurement of the step-response following a rapid change in the toroidal phase of the applied perturbations. Biorthogonal decomposition of the full set of magnetic sensors clearly defines the structures of naturally occurring external kinks as being composed of independent m/n = 3/1 and 6/2 modes. Resonant magnetic perturbations were applied to discharges with pre-existing, saturated m/n = 3/1 external kink mode activity. This m/n = 3/1 kink mode was observed to lock to the applied perturbation field. During this kink mode locked period, the plasma resonant response is characterized by a linear, a saturated, and a disruptive plasma regime dependent on the magnitude of the applied field and value of the edge safety factor and plasma rotation.We report high-resolution detection of the 3D plasma magnetic response of wall-stabilized tokamak discharges in the High Beta Tokamak-Extended Pulse [T. H. Ivers et al., Phys. Plasmas 3, 1926 (1996)] device. A new adjustable conducting wall has been installed on HBT-EP made up of 20 independent, movable, wall segments instrumented with three distinct sets of 40 modular coils that can be independently driven to generate a wide variety of magnetic perturbations. High-resolution detection of the plasma response is made with 216 poloidal and radial magnetic sensors that have been located and calibrated with high-accuracy. Static and dynamic plasma responses to resonant and non-resonant magnetic perturbations are observed through measurement of the step-response following a rapid change in the toroidal phase of the applied perturbations. Biorthogonal decomposition of the full set of magnetic sensors clearly defines the structures of naturally occurring external kinks as being composed of independent m/n = 3/1 ...
Plasma Physics and Controlled Fusion | 2015
S. Angelini; J.P. Levesque; M.E. Mauel; Gerald A. Navratil
A Phantom v7.3 fast digital camera was used to study visible light fluctuations in the High Beta Tokamak–Extended Pulse (HBT–EP). This video data is the first to be used to analyze and understand the behavior of long wavelength kink perturbations in a wall-stabilized tokamak. The light was mostly comprised of Dα 656 nm light. Profiles of the plasma light at the midplane were hollow with a radial scale length of approximately 4 cm at the plasma edge. The fast camera was also used to measure the plasmas response to applied helical magnetic perturbations. The programmed toroidal phase angle of the resonant magnetic perturbation (RMP) was directly inferred from the resulting images of the plasma response. The plasma response and the intensity of the RMP were compared under different conditions. The resulting amplitude correlations are consistent with previous measurements of the static response using an array of magnetic sensors.
Nuclear Fusion | 2013
J.P. Levesque; N. Rath; D. Shiraki; S. Angelini; J. Bialek; P.J. Byrne; B. DeBono; P.E. Hughes; M.E. Mauel; Gerald A. Navratil; Q. Peng; D.J. Rhodes; C.C. Stoafer
Plasma Physics and Controlled Fusion | 2013
N. Rath; S. Angelini; J. Bialek; P.J. Byrne; B. DeBono; P.E. Hughes; J.P. Levesque; M.E. Mauel; Gerald A. Navratil; Q. Peng; D.J. Rhodes; C.C. Stoafer
Nuclear Fusion | 2013
N. Rath; P.J. Byrne; J.P. Levesque; S. Angelini; J. Bialek; B. DeBono; P.E. Hughes; M.E. Mauel; Gerald A. Navratil; Q. Peng; D.J. Rhodes; C.C. Stoafer
Bulletin of the American Physical Society | 2014
S. Angelini
Bulletin of the American Physical Society | 2013
R. Arbacher; S. Angelini; J.P. Levesque; M.E. Mauel; G.A. Navratil; Q. Peng; D.J. Rhodes
Bulletin of the American Physical Society | 2012
S. Angelini; J.P. Levesque; M.E. Mauel; Gerald A. Navratil; S.F. Paul
Bulletin of the American Physical Society | 2011
G.A. Navratil; S. Angelini; J. Bialek; A.H. Boozer; P.J. Byrne; B. DeBono; P.E. Hughes; J.P. Levesque; L. Bi; M.E. Mauel; D.A. Maurer; Q. Peng; D.J. Rhodes; N. Rath; C. Stoaffer; D. Shiraki