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By W.M. Tang; V.S. Chan; USDOE Office of Science (SC) (US); Princeton University. Plasma Physics Laboratory.; United States. Dept. of Energy. Office of Scientific and Technical Information

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The challenge here involved applying new integrated simulation capabilities made possible by modern supercomputers. In 28 addition to efficiently combining the key physics properties from the best current theoretical models, the MPP capabilities enabled extensive campaigns of computer simulations on a huge number of designs in a short time and at low cost. New optimization software was specifically developed to allow a systematic exercising of all the relevant variables to home in on the optimal design.

Geophys. Space Phys. 13 303; Parker E N 1979 Cosmical Magnetic Fields (Oxford: Clarendon Press); Parker E N 1973 Astrophys. J. 180 247; Sato T and Hayashi T 1979 Phys. Fluids 22 1189; Biskamp D 1986 Phys. 36 Fluids 29 1520; Kulsrud R M 1998 Phys. Plasmas 5 1599; Tang W M 1998 Science 279 1488 [65] Birn J et al 2001 J. Geophys. Res. 106 3715; Aydemir A Y 1999 Phys. Fluids B 4 3469; Rogers B N et al 2001 Phys. Rev. Lett. 87 195004 [66] Yamada M et al 2000 Phys. Plasmas 7 1781; Yamada M 2001 Earth Planets Space 53 509 [67] Drake J F, Swisdak M, Cattell C, Say M A, Rogers B N and Zeiler A 2003 Science 299 873 [68] Reiman A, et al 2001 Phys.

Reduction in spurious cyclotron damping with improved poloidal mode resolution in TORIC simulation results for D (3He) mode conversion experiments in the Alcator C-Mod tokamak. 50 Figure 14. Two-dimensional field solutions for conversion of fast ion cyclotron waves to ion Bernstein waves in the heating of the DIII-D tokamak plasma. 51 Figure 15. All-orders spectral calculation of minority ion cyclotron heating for all ten field periods of the Large Helical Device (LHD) stellarator facility with a single antenna located at the extreme right-hand side.

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