C. Deng
University of Wisconsin-Madison
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Featured researches published by C. Deng.
Fusion Science and Technology | 2006
D.T. Anderson; Ali Elsayed Ali Ibrahim Abdou; A. F. Almagri; F. S. B. Anderson; J.M. Canik; W. Guttenfelder; C. Lechte; K.M. Likin; H. Lu; S. Oh; P. H. Probert; J. Radder; V. Sakaguchi; J. Schmitt; J.N. Talmadge; Kan Zhai; D. L. Brower; C. Deng
Abstract Recent results are summarized for the Helically Symmetric Experiment (HSX), which has the capability of running as a quasi-helically symmetric stellarator or as a more conventional, nonsymmetric stellarator. From X-ray measurements, we have demonstrated improved confinement of energetic particles. With central electron cyclotron heating, the density profiles in the quasi-symmetric configuration are peaked, in contrast to the hollow or flat profiles when the symmetry is broken. The difference in profiles is attributed to the lowering of the neoclassical thermodiffusive flux when the symmetry is present. The central electron temperature is ~200 eV higher for the quasi-symmetric configuration over the nonsymmetric case. The power deposition profiles are similar for the two cases, implying that the neoclassical electron thermal conductivity is reduced with quasi-symmetry. Related to the good confinement characteristics in the quasi-symmetric mode of operation, fluctuations in the density and magnetic field, consistent with that of a global Alfvén eigenmode (GAE), are observed. While the neoclassical characteristics of the quasi-symmetric and nonsymmetric configurations are very different, we have yet to find, under present operating conditions, any significant difference (other than the possible GAE mode) in turbulence characteristics or blob formation at the plasma edge.
Fusion Science and Technology | 2004
J.N. Talmadge; K.M. Likin; Ali Elsayed Ali Ibrahim Abdou; A. F. Almagri; D.T. Anderson; F. Simon B. Anderson; J.M. Canik; C. Deng; Stefan P. Gerhardt; Kan Zhai
Abstract Thomson scattering and diamagnetic loop measurements in a hot electron plasma in the Helically Symmetric Experiment (HSX) indicate that the central electron temperature and stored energy increase linearly with power. Experimentally it is found that the central electron temperature is roughly independent of plasma density. The ASTRA code is used to model electron cyclotron heating for a magnetic configuration that is quasi-symmetric as well as for a configuration in which the symmetry is broken. The experimental results are consistent with an anomalous thermal conductivity that scales inversely with the density. However, the experimental scaling of the stored energy against density is not usually in agreement with the model. From the measured X-ray flux and the high absorbed power, as well as from the calculated low single-pass absorption efficiency, it is concluded that at low densities, a nonthermal electron population accounts for a significant fraction of the stored energy. With the ASTRA code, it is also possible to model under what conditions the central electron temperature in the quasi-symmetric configuration will be measurably greater than the temperature in the nonsymmetric configuration. These calculations depend greatly on the radial electric field of the nonsymmetric plasma but suggest that at somewhat higher density and higher power than achieved to date, differences in the central electron temperature may be observed.
RADIO FREQUENCY POWER IN PLASMAS: 15th Topical Conference on Radio Frequency Power in Plasmas | 2003
K.M. Likin; J.N. Talmadge; A. F. Almagri; D.T. Anderson; F. S. B. Anderson; C. Deng; S. P. Gerhardt; Kan Zhai
Second harmonic extraordinary mode ECH is used in the HSX stellarator at 0.5 T to break down and heat the plasma. To measure the absorbed power a set of absolutely calibrated microwave diodes have been installed inside the machine. In the QHS and Mirror configuration, the absorption efficiency is high (about 0.9) and drops (to about 0.5) in the anti‐Mirror mode. A comparison with ray tracing predictions is made.
Journal of Fusion Energy | 2018
D.A. Gates; David F. Anderson; Sherwood Anderson; M. C. Zarnstorff; Donald A. Spong; Harold Weitzner; G.H. Neilson; David N. Ruzic; Daniel Andruczyk; J. H. Harris; H. Mynick; C. C. Hegna; O. Schmitz; J.N. Talmadge; Davide Curreli; D. A. Maurer; Allen H. Boozer; Stephen F. Knowlton; Jean Paul Allain; D. Ennis; G. A. Wurden; A. Reiman; J. Lore; Matt Landreman; Jeffrey P. Freidberg; S. R. Hudson; Miklos Porkolab; Diane Renee Demers; J. L. Terry; E. Edlund
Bulletin of the American Physical Society | 2017
C. Deng; D. L. Brower; D.T. Anderson; F. S. B. Anderson; K.M. Likin; J.N. Talmadge
Bulletin of the American Physical Society | 2017
J. Smoniewski; B.J. Faber; E. S 'anchez; I. Calvo; M.J. Pueschel; K.M. Likin; C. Deng; J.N. Talmadge
Bulletin of the American Physical Society | 2016
C. Deng; D. L. Brower; D.T. Anderson; F. S. B. Anderson; K.M. Likin; J.N. Talmadge
Bulletin of the American Physical Society | 2016
J.N. Talmadge; Jason Smoniewski; Konstin Likin; C. Deng; J. H. E. Proll; Harry E. Mynick; Samuel Lazerson
Bulletin of the American Physical Society | 2016
J. Smoniewski; B.J. Faber; M.J. Pueschel; K.M. Likin; C. Deng; J.N. Talmadge
Bulletin of the American Physical Society | 2015
C. Deng; D. L. Brower; D.T. Anderson; F. S. B. Anderson; K.M. Likin; J. Smoniewski; J.N. Talmadge