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Nuclear Fusion | 2007

Chapter 7: Diagnostics

A. J. H. Donné; A.E. Costley; R. Barnsley; Henrik Bindslev; R.L. Boivin; G. D. Conway; R.K. Fisher; R. Giannella; H. Hartfuss; M. von Hellermann; E. Hodgson; L. C. Ingesson; K. Itami; D.W. Johnson; Y. Kawano; T. Kondoh; A. V. Krasilnikov; Y. Kusama; A. Litnovsky; Ph. Lotte; P. Nielsen; T. Nishitani; F. Orsitto; B.J. Peterson; G. Razdobarin; J. Sánchez; M. Sasao; T. Sugie; G. Vayakis; V. S. Voitsenya

In order to support the operation of ITER and the planned experimental programme an extensive set of plasma and first wall measurements will be required. The number and type of required measurements will be similar to those made on the present-day large tokamaks while the specification of the measurements—time and spatial resolutions, etc—will in some cases be more stringent. Many of the measurements will be used in the real time control of the plasma driving a requirement for very high reliability in the systems (diagnostics) that provide the measurements. The implementation of diagnostic systems on ITER is a substantial challenge. Because of the harsh environment (high levels of neutron and gamma fluxes, neutron heating, particle bombardment) diagnostic system selection and design has to cope with a range of phenomena not previously encountered in diagnostic design. Extensive design and R&D is needed to prepare the systems. In some cases the environmental difficulties are so severe that new diagnostic techniques are required. a Author to whom any correspondence should be addressed.


Physics of Plasmas | 1999

Initial physics achievements of large helical device experiments

O. Motojima; H. Yamada; A. Komori; N. Ohyabu; K. Kawahata; O. Kaneko; S. Masuzaki; A. Ejiri; M. Emoto; H. Funaba; M. Goto; K. Ida; H. Idei; S. Inagaki; N. Inoue; S. Kado; S. Kubo; R. Kumazawa; T. Minami; J. Miyazawa; T. Morisaki; S. Morita; S. Murakami; S. Muto; T. Mutoh; Y. Nagayama; Y. Nakamura; H. Nakanishi; K. Narihara; K. Nishimura

The Large Helical Device (LHD) experiments [O. Motojima, et al., Proceedings, 16th Conference on Fusion Energy, Montreal, 1996 (International Atomic Energy Agency, Vienna, 1997), Vol. 3, p. 437] have started this year after a successful eight-year construction and test period of the fully superconducting facility. LHD investigates a variety of physics issues on large scale heliotron plasmas (R=3.9 m, a=0.6 m), which stimulates efforts to explore currentless and disruption-free steady plasmas under an optimized configuration. A magnetic field mapping has demonstrated the nested and healthy structure of magnetic surfaces, which indicates the successful completion of the physical design and the effectiveness of engineering quality control during the fabrication. Heating by 3 MW of neutral beam injection (NBI) has produced plasmas with a fusion triple product of 8×1018 keV m−3 s at a magnetic field of 1.5 T. An electron temperature of 1.5 keV and an ion temperature of 1.4 keV have been achieved. The maximum s...


Plasma Physics and Controlled Fusion | 2001

Configuration flexibility and extended regimes in Large Helical Device

H. Yamada; A. Komori; N. Ohyabu; O. Kaneko; K. Kawahata; K.Y. Watanabe; S. Sakakibara; S. Murakami; K. Ida; R. Sakamoto; Y. Liang; J. Miyazawa; Kenji Tanaka; Y. Narushima; S. Morita; S. Masuzaki; T. Morisaki; N. Ashikawa; L. R. Baylor; W.A. Cooper; M. Emoto; P.W. Fisher; H. Funaba; M. Goto; H. Idei; K. Ikeda; S. Inagaki; N. Inoue; M. Isobe; K. Khlopenkov

Recent experimental results in the Large Helical Device have indicated that a large pressure gradient can be formed beyond the stability criterion for the Mercier (high-n) mode. While the stability against an interchange mode is violated in the inward-shifted configuration due to an enhancement of the magnetic hill, the neoclassical transport and confinement of high-energy particle are, in contrast, improved by this inward shift. Mitigation of the unfavourable effects of MHD instability has led to a significant extension of the operational regime. Achievements of the stored energy of I MJ and the volume-averaged beta of 3% are representative results from this finding. A confinement enhancement factor above the international stellarator scaling ISS95 is also maintained around 1.5 towards a volume-averaged beta, (beta), of 3%. Configuration studies on confinement and MHD characteristics emphasize the superiority of the inward-shifted geometry to other geometries. The emergence of coherent modes appears to be consistent with the linear ideal MHD theory; however, the inward-shifted configuration has reduced heat transport in spite of a larger amplitude of magnetic fluctuation than the outward-shifted configuration. While neoclassical helical ripple transport becomes visible for the outward-shifted configuration in the collisionless regime, the inward-shifted configuration does not show any degradation of confinement deep in the collisionless regime (nu* < 0.1). The distinguished characteristics observed in the inward-shifted configuration help in creating a new perspective of MHD stability and related transport in net current-free plasmas. The first result of the pellet launching at different locations is also reported.


Physics of Plasmas | 2003

Formation of electron internal transport barrier and achievement of high ion temperature in Large Helical Device

Y. Takeiri; T. Shimozuma; S. Kubo; S. Morita; M. Osakabe; O. Kaneko; K. Tsumori; Y. Oka; K. Ikeda; K. Nagaoka; N. Ohyabu; K. Ida; M. Yokoyama; J. Miyazawa; M. Goto; K. Narihara; I. Yamada; H. Idei; Y. Yoshimura; N. Ashikawa; M. Emoto; H. Funaba; S. Inagaki; M. Isobe; K. Kawahata; K. Khlopenkov; T. Kobuchi; A. Komori; A. Kostrioukov; R. Kumazawa

An internal transport barrier (ITB) was observed in the electron temperature profile in the Large Helical Device [O. Motojima et al., Phys. Plasmas 6, 1843 (1999)] with a centrally focused intense electron cyclotron resonance microwave heating. Inside the ITB the core electron transport was improved, and a high electron temperature, exceeding 10 keV in a low density, was achieved in a collisionless regime. The formation of the electron-ITB is correlated with the neoclassical electron root with a strong radial electric field determined by the neoclassical ambipolar flux. The direction of the tangentially injected beam-driven current has an influence on the electron-ITB formation. For the counter-injected target plasma, a steeper temperature gradient, than that for the co-injected one, was observed. As for the ion temperature, high-power NBI (neutral beam injection) heating of 9 MW has realized a central ion temperature of 5 keV with neon injection. By introducing neon gas, the NBI absorption power was incr...


Review of Scientific Instruments | 2000

Infrared imaging video bolometer

B.J. Peterson

A new concept for an infrared imaging bolometer is proposed which provides full video (two-dimensional) imaging of the radiated power from the plasma. This concept preserves all the advantages (compared to conventional metal foil resistive bolometers) of the previously proposed and tested segmented mask infrared imaging bolometer (SIB). It avoids the problems associated with the copper mask of the SIB, while giving a full frame video image of the plasma radiation with improved experimental flexibility regarding the pixel size. Analysis of the noise equivalent power shows that compared to a SIB with the same pixel area, the infrared imaging video bolometer is 2–5 times more sensitive with improved spatial resolution. These benefits are gained at the expense of the mechanical support, which the mask provides for the foil in the SIB. A numerical algorithm is used to solve the two-dimensional heat diffusion equation for the foil and determine the time-dependent spatial distribution of incident power on the fo...


Nuclear Fusion | 2001

Energy confinement and thermal transport characteristics of net current free plasmas in the Large Helical Device

H. Yamada; K.Y. Watanabe; K. Yamazaki; S. Murakami; S. Sakakibara; K. Narihara; Kenji Tanaka; M. Osakabe; K. Ida; N. Ashikawa; P. de Vries; M. Emoto; H. Funaba; M. Goto; H. Idei; K. Ikeda; S. Inagaki; N. Inoue; M. Isobe; S. Kado; O. Kaneko; K. Kawahata; K. Khlopenkov; T. Kobuchi; A. Komori; S. Kubo; R. Kumazawa; Y. Liang; S. Masuzaki; T. Minami

The energy confinement and thermal transport characteristics of net current free plasmas in regimes with much smaller gyroradii and collisionality than previously studied have been investigated in the Large Helical Device (LHD). The inward shifted configuration, which is superior from the point of view of neoclassical transport theory, has revealed a systematic confinement improvement over the standard configuration. Energy confinement times are improved over the International Stellarator Scaling 95 by a factor of 1.6 ± 0.2 for an inward shifted configuration. This enhancement is primarily due to the broad temperature profile with a high edge value. A simple dimensional analysis involving LHD and other medium sized heliotrons yields a strongly gyro-Bohm dependence (T E Ω ρ *-3.8 ) of energy confinement times. It should be noted that this result is attributed to a comprehensive treatment of LHD for systematic confinement enhancement and that the medium sized heliotrons have narrow temperature profiles. The core stored energy still indicates a dependence of T E Ω ρ *-2.6 when data only from LIED are processed. The local heat transport analysis of discharges dimensionally similar except for ρ * suggests that the heat conduction coefficient lies between Bohm and gyro-Bohm in the core and changes towards strong gyro-Bohm in the peripheral region. Since the inward shifted configuration has a geometrical feature suppressing neoclassical transport, confinement improvement can be maintained in the collisionless regime where ripple transport is important. The stiffness of the pressure profile coincides with enhanced transport in the peaked density profile obtained by pellet injection.


Plasma Physics and Controlled Fusion | 2003

Formation of electron internal transport barriers by highly localized electron cyclotron resonance heating in the large helical device

T. Shimozuma; S. Kubo; H. Idei; Y. Yoshimura; T. Notake; K. Ida; N. Ohyabu; I. Yamada; K. Narihara; S. Inagaki; Y. Nagayama; Y. Takeiri; H. Funaba; S. Muto; Kenji Tanaka; M. Yokoyama; S. Murakami; M. Osakabe; R. Kumazawa; N. Ashikawa; M. Emoto; M. Goto; K. Ikeda; M. Isobe; T Kobichi; Y. Liang; S. Masuzaki; T. Minami; J. Miyazawa; S. Morita

Internal transport barriers with respect to electron thermal transport (eITB) were observed in the large helical device, when the electron cyclotron resonance heating (ECH) power was highly localized on the centre of a plasma sustained by neutral beam injection. The eITB is characterized by a high central electron temperature of 6–8 keV with an extremely steep gradient, as high as 55 keV m−1 and a low electron thermal diffusivity within a normalized average radius ρ≈0.3 as well as by the existence of clear thresholds for the ECH power and plasma collisionality.


Plasma Physics and Controlled Fusion | 2003

Bolometer diagnostics for one- and two-dimensional measurements of radiated power on the Large Helical Device

B.J. Peterson; A Yu Kostrioukov; N. Ashikawa; Yi Liu; Yuhong Xu; Masaki Osakabe; K Y Watanabe; T Shimozuma; S. Sudo

Bolometer diagnostics are installed on the Large Helical Device (LHD) to provide measurements of the total (broad spectrum) electromagnetic radiation emitted by the plasma. Three types of detectors are used: resistive metal film bolometers, absolute extreme ultraviolet photodiodes and infrared imaging video bolometers. Details of the installation in LHD are given for each type of detector. The detector calibration, data analysis and tomography techniques are described and compared and sample results are shown.


Nuclear Fusion | 2001

MHD characteristics in the high beta regime of the Large Helical Device

S. Sakakibara; H. Yamada; K.Y. Watanabe; Y. Narushima; K. Toi; S. Ohdachi; M. Takechi; Satoshi Yamamoto; K. Narihara; Kenji Tanaka; N. Ashikawa; P. de Vries; M. Emoto; H. Funaba; M. Goto; K. Ida; H. Idei; K. Ikeda; S. Inagaki; N. Inoue; M. Isobe; S. Kado; O. Kaneko; K. Kawahata; K. Khlopenkov; T. Kobuchi; A. Komori; S. Kubo; R. Kumazawa; Y. Liang

Note: Proc. 18th IAEA Fusion Energy Conference, Sorrento, Italy, 4-10 October 2000, IAEA-CN-77 (EXP3/12), p. 157 (2000) Reference CRPP-CONF-2000-073 Record created on 2008-05-13, modified on 2017-05-12


Nuclear Fusion | 1999

Confinement physics study in a small low aspect ratio helical device: CHS

S. Okamura; K. Matsuoka; R. Akiyama; D. S. Darrow; A. Ejiri; A. Fujisawa; M. Fujiwara; M. Goto; K. Ida; H. Idei; H. Iguchi; N. Inoue; M. Isobe; K. Itoh; S. Kado; K. Khlopenkov; T. Kondo; S. Kubo; A. Lazaros; S. Lee; G. Matsunaga; T. Minami; S. Morita; S. Murakami; Noriyoshi Nakajima; N. Nikai; S. Nishimura; I. Nomura; S. Ohdachi; K. Ohkuni

Variation of the plasma position relative to the centre of the helical coil winding is a very effective means of controlling the MHD stability and the trapped particle confinement in heliotron/torsatron systems, but improving one of these two characteristics with this parameter simultaneously has a detrimental effect on the other. The inward shifted configuration is favourable for drift orbit optimization but is predicted to be unstable according to the Mercier criterion. Various physics problems, such as electric field structure, plasma rotation and MHD phenomena, have been studied in the Compact Helical System (CHS) with a compromise intermediate position. With this standard configuration, CHS has yielded experimental results that contribute to the understanding of general toroidal confinement physics and low aspect ratio helical systems. In the recent experiments, it was found that a wide range of inward shifted configurations give stable plasma discharges without any restriction to the special pressure profile. Such an enhanced range of operation made it possible to study experimentally the drift orbit optimized configuration in heliotron/torsatron systems. The effect of configuration improvement was studied with plasmas in a low collisionality regime.

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S. Masuzaki

Graduate University for Advanced Studies

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H. Funaba

Graduate University for Advanced Studies

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N. Ashikawa

Graduate University for Advanced Studies

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K. Narihara

Graduate University for Advanced Studies

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K. Kawahata

Budker Institute of Nuclear Physics

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J. Miyazawa

Graduate University for Advanced Studies

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